WorldWideScience

Sample records for temperature magnetocaloric effect

  1. Magnetocaloric effect at cryogenic temperature in gadolinium oxide nanotubes

    Energy Technology Data Exchange (ETDEWEB)

    Paul, Rima, E-mail: rima.paul@saha.ac.in [Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Kolkata 700064 (India); Paramanik, Tapas; Das, Kalipada [Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Kolkata 700064 (India); Sen, Pintu [Variable Energy Cyclotron Centre, 1/AF Bidhannagar, Kolkata 700064 (India); Satpati, B.; Das, I. [Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Kolkata 700064 (India)

    2016-11-01

    We have synthesized fascinating nano-structure of Gadolinium oxide (Gd{sub 2}O{sub 3}) using controlled template-assisted electrochemical deposition technique which showed interesting anisotropic magnetic behavior. The nanotubes of Gd{sub 2}O{sub 3} with average diameter 200 nm, length 10 µm and wall thickness 20 nm are constituted of nanoclusters with average diameter 7.5 nm. The tubes are aligned and are almost uniform throughout their length. Detailed magnetic measurements of aligned Gd{sub 2}O{sub 3} nanotubes have been performed for both parallel and perpendicular magnetic field orientations with respect to the axis of the Gd{sub 2}O{sub 3} nanotube array. Significant differences in magnetization values have been observed between the parallel and perpendicular orientations. Experimental results indicate the superparamagnetic nature of the nanomaterial. Large magnetocaloric effect, associated with the sharp change in magnetization of the Gd{sub 2}O{sub 3} nanotubes, has been observed in the cryogenic temperature regime that shows anisotropic behavior. - Highlights: • Gd{sub 2}O{sub 3} nanotubes of diameter ~200 nm synthesized through electrochemical technique. • The nanotubes are superparamagnetic in nature. • At cryogenic temperature, the nanotubes exhibit large magnetocaloric anisotropic effect.

  2. Magnetocaloric effect in temperature-sensitive magnetic fluids

    Indian Academy of Sciences (India)

    The magnetocaloric properties of three different temperature-sensitive magnetic fluids were studied. The pyromagnetic coefficient for all the materials were obtained and it was found that this property depends on physical and magnetic properties like size, magnetization and Curie temperature. A theoretical model was ...

  3. Magnetocaloric effect in temperature-sensitive magnetic fluids

    Indian Academy of Sciences (India)

    Unknown

    magnetization, heat capacity of the material and carrier liquid. In this paper, we report the magnetocaloric pro- perties of certain temperature-sensitive magnetic fluids. Here, an indirect measurement technique to determine the change in entropy using temperature-dependent magnetic property of magnetic fluid, is reported.

  4. Compositional invariance of magnetocaloric effect near room temperature in Ni-Mn-Sb-Al systems

    Science.gov (United States)

    Agarwal, Sandeep; Mukhopadhyay, P. K.

    2018-02-01

    A systematic study of structural transformation, magnetism and magnetic entropy change in the vicinity of structural and magnetic transformation has been performed in the Ni2Mn1.36Sb0.64 by substituting Sb with a large amount of Al. This substitution enhanced the transformation temperature close to room temperature and also made it less sensitive to the variation in composition. Alloys exhibited conventional and inverse magnetocaloric effects due to the Curie and magnetostructural transformation respectively. The inverse magnetocaloric effects were less compared to those reported in pure Sb system, but it showed a large value of conventional magnetocaloric effect with the added advantage of insensitivity to the compositional variation.

  5. Large magnetocaloric effect in geometrically frustrated polycrystalline ErMnO3 compound at cryogenic temperature

    Science.gov (United States)

    Das, Kalipada; Banik, Sanjib; Das, I.

    2018-03-01

    In this manuscript we report significantly large magnetocaloric effect in the cryogenic temperature region for the chemically stable polycrystalline ErMnO3 compound. For this compound, the antiferromagnetic transition temperature of the Mn3+ ions is nearly T ∼ 75 K. However, the large non saturating magnetization and magnetocaloric effect are found at a temperature lower than 20 K. Such non saturating nature of magnetization and magnetic entropy changes for the application of external magnetic field is addressed by considering the gradual alignments of dominant paramagnetic moments caused by Er3+ ions.

  6. Constraints on the Adiabatic Temperature Change in Magnetocaloric Materials

    DEFF Research Database (Denmark)

    Nielsen, Kaspar Kirstein; Bahl, Christian Robert Haffenden; Smith, Anders

    2010-01-01

    The thermodynamics of the magnetocaloric effect implies constraints on the allowed variation in the adiabatic temperature change for a magnetocaloric material. An inequality for the derivative of the adiabatic temperature change with respect to temperature is derived for both first- and second...

  7. FAST TRACK COMMUNICATION: Reproducible room temperature giant magnetocaloric effect in Fe-Rh

    Science.gov (United States)

    Manekar, Meghmalhar; Roy, S. B.

    2008-10-01

    We present the results of magnetocaloric effect (MCE) studies in polycrystalline Fe-Rh alloy over a temperature range of 250-345 K across the first order antiferromagnetic to ferromagnetic transition. By measuring the MCE under various thermomagnetic histories, contrary to the long held belief, we show here explicitly that the giant MCE in Fe-Rh near room temperature does not vanish after the first field cycle. In spite of the fact that the virgin magnetization curve is lost after the first field cycle near room temperature, reproducibility in the MCE under multiple field cycles can be achieved by properly choosing a combination of isothermal and adiabatic field variation cycles in the field-temperature phase space. This reproducible MCE leads to a large effective refrigerant capacity of 324.42 J kg-1, which is larger than that of the well-known magnetocaloric material Gd5Si2Ge2. This information could be important as Fe-Rh has the advantage of having a working temperature of around 300 K, which can be used for room temperature magnetic refrigeration.

  8. Calculation model on magnetocaloric effect (MCE) and relative cooling power (RCP) in composite materials at room temperature

    Science.gov (United States)

    El Hafidi, Moulay Youssef; Boubekri, Abderrazzak; El Hafidi, Mohamed

    2018-03-01

    In this paper, a calculation model is proposed to measure magnetocaloric effect (MCE) and relative cooling power (RCP) in composites based on magnetic materials underscoring a giant MCE at room temperature. The two composite materials targeted are Gd-Gd5Si2Ge2 and MnAs-Mn1+δAs0.9Sb0.1 due to their high magnetic entropy change ΔSM over 270-300 K and 280-320 K. Our selected composites could give a larger RCP value among existing magnetocaloric materials for magnetic refrigeration in the temperature range of 280-300 K which is desirable for ideal Ericsson-cycle magnetic refrigeration. The excellent magnetocaloric properties of these two magnetic composites make them attractive for active magnetic refrigeration at room temperature.

  9. New type of magnetocaloric effect: Implications on low-temperature magnetic refrigeration using an Ericsson cycle

    International Nuclear Information System (INIS)

    Takeya, H.; Pecharsky, V.K.; Gschneidner, K.A. Jr.; Moorman, J.O.

    1994-01-01

    The low-temperature, high magnetic field heat capacity (1.5 to 70 K and 0 to 9.85 T), dc and ac magnetic behaviors of the compound (Gd 0.54 Er 0.46 )AlNi show that field-induced magnetic entropy change is significant and almost constant over the temperature region of ∼15 to ∼45 K. The resulting temperature dependence of the magnetocaloric effect, nearly constant over a 30+ K temperature range, is unprecedented (most magnetic materials have a caretlike shape temperature dependence). These data show that (Gd 0.54 Er 0.46 )AlNi can be used as an effective active magnetic regenerator material for an Ericsson-cycle magnetic refrigerator, and could substitute for complex composite layered materials suggested earlier

  10. Understanding the inverse magnetocaloric effect in antiferro- and ferrimagnetic arrangements

    International Nuclear Information System (INIS)

    Von Ranke, P J; De Oliveira, N A; Alho, B P; Plaza, E J R; De Sousa, V S R; Caron, L; Reis, M S

    2009-01-01

    The inverse magnetocaloric effect occurs when a magnetic material cools down under applied magnetic field in an adiabatic process. Although the existence of the inverse magnetocaloric effect was recently reported experimentally, a theoretical microscopic description is almost nonexistent. In this paper we theoretically describe the inverse magnetocaloric effect in antiferro- and ferrimagnetic systems. The inverse magnetocaloric effects were systematically investigated as a function of the model parameters. The influence of the Neel and the compensation temperature on the magnetocaloric effect is also analyzed using a microscopic model.

  11. Understanding the inverse magnetocaloric effect in antiferro- and ferrimagnetic arrangements

    Energy Technology Data Exchange (ETDEWEB)

    Von Ranke, P J; De Oliveira, N A; Alho, B P; Plaza, E J R; De Sousa, V S R [Instituto de Fisica ' Armando Dias Tavares' , Universidade do Estado do Rio de Janeiro-UERJ, Rua Sao Francisco Xavier, 524, 20550-013, RJ (Brazil); Caron, L [Instituto de Fisica ' Gleb Wataghin' , Universidade Estadual de Campinas-UNICAMP, 13083-970 Campinas, SP (Brazil); Reis, M S [CICECO, Universidade de Aveiro, 3810-193 Aveiro (Portugal)], E-mail: von.ranke@uol.com.br

    2009-02-04

    The inverse magnetocaloric effect occurs when a magnetic material cools down under applied magnetic field in an adiabatic process. Although the existence of the inverse magnetocaloric effect was recently reported experimentally, a theoretical microscopic description is almost nonexistent. In this paper we theoretically describe the inverse magnetocaloric effect in antiferro- and ferrimagnetic systems. The inverse magnetocaloric effects were systematically investigated as a function of the model parameters. The influence of the Neel and the compensation temperature on the magnetocaloric effect is also analyzed using a microscopic model.

  12. Magnetocaloric effect in temperature-sensitive magnetic fluids

    Indian Academy of Sciences (India)

    Unknown

    Magnetic fluid; pyromagnetic coefficient; Curie temperature. 1. Introduction. A magnetic fluid also known as a ferrofluid is a suspen- sion of nanosize ferromagnetic or ferrimagnetic particles in a carrier liquid. Upon application of magnetic field, the entropy associated with the magnetic degree of freedom is changed due to the ...

  13. Room temperature magnetocaloric effect in Ni-Mn-In-Cr ferromagnetic shape memory alloy thin films

    Energy Technology Data Exchange (ETDEWEB)

    Akkera, Harish Sharma [Functionalnanomaterials Research Lab, Department of Physics, Indian Institute of Technology Roorkee, Uttarakhand-247667 (India); Singh, Inderdeep [Mechanical and Industrial Engineering Department, Indian Institute of Technology Roorkee, Uttarakhand-24667 (India); Kaur, Davinder, E-mail: dkaurfph@iitr.ernet.in [Functionalnanomaterials Research Lab, Department of Physics, Indian Institute of Technology Roorkee, Uttarakhand-247667 (India)

    2017-02-15

    The influence of Cr substitution for In on the martensitic phase transformation and magnetocaloric effect (MCE) has been investigated in Ni-Mn-Cr-In ferromagnetic shape memory alloy (FSMA) thin films fabricated by magnetron sputtering. Temperature dependent magnetization (M-T) measurements demonstrated that the martensitic transformation temperatures (T{sub M}) monotonously increase with the increase of Cr content due to change in valence electron concentration (e/a) and cell volume. From the study of isothermal magnetization curves (M-H), magnetocaloric effect around the martensitic transformation has been investigated in these FSMA thin films. The magnetic entropy change ∆S{sub M} of 7.0 mJ/cm{sup 3}-K was observed in Ni{sub 51.1}Mn{sub 34.9}In{sub 9.5}Cr{sub 4.5} film at 302 K in an applied field of 2 T. Further, the refrigerant capacity (RC) was also calculated for all the films in an applied field of 2 T. These findings indicate that the Cr doped Ni-Mn-In FSMA thin films are potential candidates for room temperature micro-length-scale magnetic refrigeration applications. - Highlights: • The Cr content leads to an increase in the martensitic transformation temperature. • The ∆S{sub M} =7 mJ/cm{sup 3}-K at 302 K was observed in the Ni{sub 51.1}Mn{sub 34.9}In{sub 9.5}Cr{sub 4.5}. • The RC =39.2 mJ/K at 2 T was obtained in Ni{sub 51.1}Mn{sub 34.9}In{sub 9.5}Cr{sub 4.5} film.

  14. Quantification of the effect of hysteresis on the adiabatic temperature change in magnetocaloric materials

    DEFF Research Database (Denmark)

    von Moos, Lars; Bahl, Christian R.H.; Nielsen, Kaspar Kirstein

    2014-01-01

    We quantify the effect of hysteresis on the performance of the magnetocaloric first order material Gd5Si2Ge2 undergoing an ideal active magnetic regenerator (AMR) cycle. The material is carefully characterized through magnetometry (VSM) and calorimetry (DSC) in order to enable an accurate model...

  15. Understanding the inverse magnetocaloric effect through a simple theoretical model

    Energy Technology Data Exchange (ETDEWEB)

    Ranke, P.J. von, E-mail: von.ranke@uol.com.b [Instituto de Fisica Armando Dias Tavares-Universidade do Estado do Rio de Janeiro, Rua Sao Francisco Xavier, 524, Rio de Janeiro 20550-013 (Brazil); Alho, B.P.; Nobrega, E.P.; Oliveira, N.A. de [Instituto de Fisica Armando Dias Tavares-Universidade do Estado do Rio de Janeiro, Rua Sao Francisco Xavier, 524, Rio de Janeiro 20550-013 (Brazil)

    2009-10-15

    We investigated the inverse magnetocaloric effect using a theoretical magnetic model formed by two coupled magnetic lattices to describe a ferrimagnetic system. The influence of the compensation temperature, and the ferrimagnetic-paramagnetic phase transition on the magnetocaloric effect was analyzed. Also, a relation between the area under the magnetocaloric curve and the net magnetic moment of a ferrimagnetic system was established in this work.

  16. Magnetic Refrigeration and the Magnetocaloric Effect

    DEFF Research Database (Denmark)

    Petersen, Thomas Frank; Pryds, Nini; Smith, Anders

    2006-01-01

    Magnetic refrigeration at room temperature is an emerging technology for refrigeration, which promises low energy consumption and is environmentalle friendly. Magnetic refrigeration is based on the magnetocaloric effect, which manifests itself as a reversibel increase in temperature when magnetic...... material are plased in a magnetic field. This paper introduces and describes magnetic refrigeration cycles and the magnetocaloric effect, and shows how magnetic refrigeration can be an alternative to vapour-compression refrigeration,. A review of the Danish research on magnetic refrigeration at Risø...

  17. Evaluating the effect of magnetocaloric properties on magnetic refrigeration performance

    DEFF Research Database (Denmark)

    Engelbrecht, Kurt; Bahl, Christian Robert Haffenden

    2010-01-01

    Active magnetic regenerator (AMR) refrigerators represent an alternative to vapor compression technology that relies on the magnetocaloric effect in a solid refrigerant. Magnetocaloric materials are in development and properties are reported regularly. Recently, there has been an emphasis...... the performance of a practical system. The distribution of the magnetocaloric effect as a function of temperature was also studied. It was found that the adiabatic temperature change in a magnetocaloric material can be more important than the isothermal entropy change for certain conditions. A material...... on developing materials with a high entropy change with magnetization while placing lower emphasis on the adiabatic temperature change. This work uses model magnetocaloric materials and a numerical AMR model to predict how the temperature change and entropy change with magnetization interact and how they affect...

  18. Magnetocaloric effect across the coupled structural and ...

    Indian Academy of Sciences (India)

    Wintec

    MCE is change in temperature of a magnetic material in adiabatic condition as a result of the alignment of its magnetic spins on exposure to an external magnetic field, the phenomenon which forms the basis for magnetic refrigeration. A large magnetocaloric effect was reported near room tem- perature in Gd and its alloys ...

  19. Giant magnetocaloric effect in isostructural MnNiGe-CoNiGe system by establishing a Curie-temperature window

    KAUST Repository

    Liu, E. K.

    2013-03-28

    An effective scheme of isostructural alloying was applied to establish a Curie-temperature window in isostructural MnNiGe-CoNiGe system. With the simultaneous accomplishment of decreasing structural-transition temperature and converting antiferromagnetic martensite to ferromagnetic state, a 200 K Curie-temperature window was established between Curie temperatures of austenite and martensite phases. In the window, a first-order magnetostructural transition between paramagnetic austenite and ferromagnetic martensite occurs with a sharp jump in magnetization, showing a magnetic entropy change as large as −40 J kg−1 K−1 in a 50 kOe field change. This giant magnetocaloric effect enables Mn1− x Co x NiGe to become a potential magnetic refrigerant.

  20. The universal behavior of inverse magnetocaloric effect in antiferromagnetic materials

    Science.gov (United States)

    Biswas, Anis; Chandra, Sayan; Samanta, Tapas; Phan, M. H.; Das, I.; Srikanth, H.

    2013-05-01

    We report the universal behavior of inverse magnetocaloric effect (IMCE) in antiferromagnetic materials. In contrast to the universal behavior of conventional magnetocaloric effect often observed in ferromagnetic systems, a phenomenological universal master curve can be constructed to describe the temperature dependence of magnetic entropy change for IMCE without rescaling the temperature axis. The proposed universal curve method allows extrapolating the magnetic entropy change of an IMCE material, which would be imperative to judge its suitability in actual magnetic refrigeration devices.

  1. The effect of different minor additions on the magneto-caloric effect of FeZrB metallic ribbons near room temperature

    Science.gov (United States)

    Guo, D. Q.; Yuan, Y. D.; Chan, K. C.

    2018-01-01

    For room-temperature magnetic refrigerators, magnetocaloric materials are critical for their performance and reliability. Among various magnetocaloric materials, Fe-based metallic glasses, especially in the FeZrB system, have been intensively studied recently due to their promising properties such as low fabrication cost and broad magnetic entropy change peak. In order to further improve the magnetocaloric effect (MCE), the influence of minor additions of Co, Er, Sm and Mn on the MCE of FeZrB-based metallic glasses was systematically investigated in this work. The composition-dependent Curie temperatures (TC) were studied and the magnetic field-dependent MCE was investigated. In two compositions, Fe88Zr7B3Co2 and Fe86Zr8B4Sm2, it was found that their Curie temperatures were close to room temperature and the values of the refrigerant capacity and peak magnetic entropy change were larger than those reported for Fe-based metallic glass at room temperature.

  2. Magnetocaloric effect of thin Terbium films

    Science.gov (United States)

    Mello, V. D.; Anselmo, D. H. A. L.; Vasconcelos, M. S.; Almeida, N. S.

    2017-12-01

    We report a theoretical study of the magnetocaloric effect of Terbium (Tb) thin films due to finite size and surface effects in the helimagnetic phase, corresponding to a temperature range from TC=219 K to TN=231 K, for external fields of the order of kOe. For a Tb thin film of 6 monolayers submitted to an applied field (ΔH =30 kOe, ΔH =50 kOe and ΔH = 70 kOe) we report a significative change in adiabatic temperature, ΔT / ΔH , near the Néel temperature, of the order ten times higher than that observed for Tb bulk. On the other hand, for small values of the magnetic field, large thickness effects are found. For external field strength around few kOe, we have found that the thermal caloric efficiency increases remarkably for ultrathin films. For an ultrathin film with 6 monolayers, we have found ΔT / ΔH = 43 K/T while for thicker films, with 20 monolayers, ΔT / ΔH = 22 K/T. Our results suggest that thin films of Tb are a promising material for magnetocaloric effect devices for applications at intermediate temperatures.

  3. Magnetic properties and magnetocaloric effect at room temperature of Ni50- x Ag x Mn37Sn13 alloys

    Science.gov (United States)

    Thanh, Tran Dang; Mai, Nguyen Thi; Dan, Nguyen Huy; Phan, The-Long; Yu, Seong-Cho

    2014-11-01

    In this work, we present a detailed study of the magnetic properties and the magnetocaloric effect at room temperature of Ni50- x Ag x Mn37Sn13 alloys with x = 1, 2, and 4, which were prepared by using an arc-melting method. Experimental results reveal that a partial replacement of Ag for Ni leads to a decrease in the anti-FM phase in the alloys. In addition, the martensitic-austenitic phase transition shifts towards lower temperature and is broaded. The Curie temperature ( T C A ) for the austenitic phase also shifts toward to lower temperature, but not by much. The Curie temperature was found to be 308, 305, and 298 K for x = 1, 2, and 4, respectively. The magnetic entropy change (Δ S m ) of the samples was calculated by using isothermal magnetization data. Under an applied magnetic field change of 10 kOe, the maximum value of Δ S m (|Δ S max |) was achieved at around room temperature and did not change much (~0.8 J·kg-1·K-1) with increasing Ag-doping concentration. Particularly, the M 2 vs. H/ M curves prove that all the samples exhibited a second-order magnetic phase transition. Based on Landau's phase-transition theory and careful analyses of the magnetic data around the T C A , we have determined the critical parameters β, γ, δ, and T C . The results show that the β values are located between those expected for the 3D-Heisenberg model ( β = 0.365) and mean-field theory ( β = 0.5). Such a result proves the coexistence of short-range and long-range ferromagnetic interactions in Ni50- x Ag x Mn37Sn13 alloys. The nature of the changes in the critical parameters and the |Δ S max | is thoroughly discussed by means of structural analyses.

  4. Large Magnetocaloric Effect Around Room Temperature in Amorphous Fe-Gd-Zr Alloy Ribbon with Short-Range Interactions

    Science.gov (United States)

    Thanh, Tran Dang; Yen, Nguyen Hai; Duc, Nguyen Huu; Phan, The-Long; Dan, Nguyen Huy; Yu, Seong-Cho

    2016-05-01

    In this work, we present a detailed study on the magnetocaloric effect and the critical behaviors of an amorphous Fe88Gd2Zr10 alloy ribbon prepared by using a rapid quenching method. We point out that the value of maximum magnetic entropy change (|Δ S max|) of amorphous Fe88Gd2Zr10 alloy ribbon appeared at near room temperature and versus Δ H obeys a power law, |Δ S max| = a·Δ H n. In addition, all Δ S m( T, Δ H) data measured at different Δ H values are collapsed onto a universal master curve. Interestingly, M 2 versus H/ M curves prove amorphous Fe88Gd2Zr10 ribbon exhibitied a second-order magnetic phase transition. The critical exponents ( β, γ, and δ) obtained from the modified Arrott plots and the Kouvel-Fisher methods, and critical isotherm analysis are very close to those expected for the 3D-Heisenberg model, proving ferromagnetic short-range interactions exist in amorphous Fe88Gd2Zr10 ribbon.

  5. Magnetocaloric effect in rare-earth intermetallics: Recent trends

    Indian Academy of Sciences (India)

    cooling [1,2]. For these reasons, extensive research is being carried out to identify suitable magnetic materials for their use as magnetic refrigerants in various temperature ranges. Magnetocaloric effect (MCE) is the change in isothermal magnetic entropy ( Sm) and adiabatic temperature ( Tad) that accompany magnetic ...

  6. Magnetocaloric effect of Gd 5 Si 2 Ge 2 alloys in low magnetic field

    Indian Academy of Sciences (India)

    The magnetocaloric effect (MCE) is studied by measuring magnetic entropy change ( M) and adiabatic temperature change ( ad) in a magnetic field of 1.5 T using a vibrating sample magnetometer (VSM) and a home-made magnetocaloric effect measuring apparatus, respectively. The maximum M of the alloys ...

  7. Magnetocaloric effect of Gd5 Si2 Ge2 alloys in low magnetic field

    Indian Academy of Sciences (India)

    Administrator

    low magnetic fields. The magnetocaloric effect (MCE) is studied by measuring magnetic entropy change (ΔSM) and adiabatic temperature change (ΔTad) in a magnetic field of 1⋅5 T using a vibrating sample magnetometer. (VSM) and a home-made magnetocaloric effect measuring apparatus, respectively. The maximum ...

  8. A large reversible room temperature magneto-caloric effect in Ni-TM-Co-Mn-Sn (TM = Ti, V, Cr) meta-magnetic Heusler alloys

    Science.gov (United States)

    Kim, S. J.; Ryu, W. H.; Oh, H. S.; Park, E. S.

    2018-01-01

    Herein, we achieved a large reversible room temperature magneto-caloric effect (MCE) through synergic tuning of martensitic transformation (MT) temperatures and transition entropy change (ΔStr) via micro-alloying with transition metals (Ti, V, and Cr) in Ni45Co5Mn40Sn10 meta-magnetic Heusler alloys (MHAs). By the minor addition of TM, MT temperatures were brought down to below room temperature and ΔStr was reduced while maintaining narrow MT temperature range (ΔT) and large difference in magnetization (ΔM) of Ni45Co5Mn40Sn10 MHA. In particular, Ni43.8Cr1.2Co5Mn40Sn10 MHA exhibited a very large reversible room temperature magnetic entropy change (ΔSM) of 24.5 J/kg.K with a broad operating temperature window of ˜11 K at 5 T. Indeed, the MHA exhibited a very effective refrigeration capacity (RCeff) of 276 J/kg for 5 T, which is the largest value among the reported Ni-Mn-based MHAs. The decrease of ΔStr reduces the magnetic field required for completely reversible MT and accelerates the saturation of ΔSM, which leads to maximum RCeff value in the composition of MHA. Thus, we can conclude that smaller ΔStr with narrow ΔT and large ΔM is a key variable to develop MHA with reversible MCE under low magnetic field, which will ultimately give us a guideline for the tailor-made design of high-performance magneto-caloric materials.

  9. Magnetocaloric effects of ferromagnetic erbium mononitride

    Energy Technology Data Exchange (ETDEWEB)

    Nakagawa, Takashi [Graduate School of Engineering, Osaka University, Suita, Osaka 565-0871 (Japan)]. E-mail: nakagawa@mit.eng.osaka-u.ac.jp; Arakawa, Takayuki [Graduate School of Engineering, Osaka University, Suita, Osaka 565-0871 (Japan); Sako, Kengo [Graduate School of Engineering, Osaka University, Suita, Osaka 565-0871 (Japan); Tomioka, Naoto [Graduate School of Engineering, Osaka University, Suita, Osaka 565-0871 (Japan); Yamamoto, Takao A. [Graduate School of Engineering, Osaka University, Suita, Osaka 565-0871 (Japan); Kusunose, Takafumi [Institute of Scientific and Industrial Research, Osaka University, Ibaraki 567-0047 (Japan); Niihara, Koichi [Institute of Scientific and Industrial Research, Osaka University, Ibaraki 567-0047 (Japan); Kamiya, Koji [Tsukuba Magnet Laboratory, National Institute for Materials Science, Tsukuba, Ibaraki 305-0003 (Japan); Numazawa, Takenori [Tsukuba Magnet Laboratory, National Institute for Materials Science, Tsukuba, Ibaraki 305-0003 (Japan)

    2006-02-09

    The rare earth mononitride, ErN, has been synthesized by the carbothermic reduction and hot isostatic press methods. The magnetocaloric effect of ErN has been evaluated by calculating the magnetic entropy changes, {delta}S, from the magnetization data sets and from the heat capacity measured at various temperatures and applied fields. The two results are in good agreement with each other. The {delta}S value of ErN is the highest at 7.5 K and higher than that of ErNi{sub 2} reported as the candidate material for the magnetic refrigerant of cryogenic technology. Heat capacity curve against temperature of ErN has a peak at 4.4 K at zero-field. The peak value of the heat capacity of ErN is 507 kJ K{sup -1} m{sup -3}. This value is larger than those of Er{sub 3}Ni used commercially as a magnetic regenerator for the Gifford-McMahon refrigerator. The present results indicate that ErN is a promising material for the magnetic refrigerant and regenerator of cooling systems working above the boiling temperature of helium.

  10. A novel magnetic valve using room temperature magnetocaloric materials

    DEFF Research Database (Denmark)

    Eriksen, Dan; Bahl, Christian; Pryds, Nini

    2012-01-01

    Magnetocaloric materials with near-room-temperature tuneable Curie temperatures have been utilized to develop a novel magnetic valve technology. The temperature dependent attractive force between the materials and a permanent magnet assembly is used to actuate valves as a response to temperature...... changes. This is made possible by the strong temperature dependence of the magnetization close to the Curie temperature of the magnetocaloric materials. Different compositions of both La0.67(Ca,Sr)0.33MnO3 and La(Fe,Co,Si)13 have been considered for use in prototype valves. Based on measured magnetization...... data a 3D finite element model has been set up to calculate the magnetic force between (graded) blocks of these materials and a permanent magnet assembly. The results have been used to calculate equilibrium points for actuation systems where the magnetic force is balanced by a spring force...

  11. Towards enhanced magnetocaloric effects: a combined experimental / computational methodology

    Science.gov (United States)

    Sandeman, Karl

    2014-03-01

    A simple thermodynamic analysis shows that there is scope to double the adiabatic temperature change of d-metal magnetocaloric materials in a fixed change of magnetic field. If found in a a real material, such an improvement in the MCE will have two important effects: to increase the final efficiency of the cooling device and to reduce the use of rare earth materials in the magnet that is used to drive the MCE. I will give examples of a methodology for the search for new magnetocaloric materials, combining neutron scattering studies with materials modelling. We have used this approach to understand magneto-elastic coupling at a fundamental level in both Mn-based and Fe-based tricritical metamagnets. Financial support is acknowledged from The Royal Society and EPSRC grant EP/G060940/1. The research leading to these results has received funding from the European Community's 7th Framework Programme under Grant agreement 310748, DRREAM.

  12. Na-doped La0.7Ca0.3MnO3 compounds exhibiting a large magnetocaloric effect near room temperature

    Science.gov (United States)

    Chi Linh, Dinh; Thi Ha, Nguyen; Huu Duc, Nguyen; Giang Nam, Le Huu; Bau, Le Viet; Manh An, Nguyen; Yu, Seong-Cho; Dang Thanh, Tran

    2018-03-01

    In this work, we have investigated the magnetic properties and the magnetocaloric effect of La0.7-xNaxCa0.3MnO3 compounds, which were prepared by a conventional solid-state reaction technique. The Rietveld refinement results suggested that the samples are single phase belonging to an orthorhombic structure (space group Pnma). Analyzing temperature dependence of magnetization M(T) revealed that the Curie temperature (TC) increases with increasing Na content (x). Their TC value is found to be 260-298 K for x=0.0-0.1, respectively. Base on M(T) data measured at different applied magnetic fields (H), temperature dependence of magnetic entropy change ΔSm(T) data for all the samples was calculated by using a phenomenological model. In the vicinity of TC, -ΔSm(T) curve reaches a maximum value (denoted as |ΔSmax|), which gradually increases with increasing H. Under 12 kOe, the value of |ΔSmax| is in a range of 1.47-5.19 J/kg K corresponding to the relative cooling power RCP=57.12-75.88 J/kg. Applied the universal master curve method for the magnetic entropy change, we concluded that Na-doped in La0.7-xNaxCa0.3MnO3 compounds leads to modification the nature of the magnetic phase transition from the first- to the second-order.

  13. Measuring the effect of demagnetization in stacks of gadolinium plates using the magnetocaloric effect

    DEFF Research Database (Denmark)

    Lipsø, Hans Kasper Wigh; Nielsen, Kaspar Kirstein; Christensen, Dennis

    2011-01-01

    The effect of demagnetization in a stack of gadolinium plates is determined experimentally by using spatially resolved measurements of the adiabatic temperature change due to the magnetocaloric effect. The number of plates in the stack, the spacing between them and the position of the plate...

  14. Investigation on the magnetocaloric effect in TbN compound

    Energy Technology Data Exchange (ETDEWEB)

    Ranke, P.J. von, E-mail: von.ranke@uol.com.br [Instituto de Física, Universidade do Estado do Rio de Janeiro—UERJ, Rua São Francisco Xavier, 524, 20550-013 RJ (Brazil); Alvarenga, T.S.T.; Nóbrega, E.P.; Alho, B.P.; Ribeiro, P.O. [Instituto de Física, Universidade do Estado do Rio de Janeiro—UERJ, Rua São Francisco Xavier, 524, 20550-013 RJ (Brazil); Carvalho, A. Magnus G. [Divisão de Metrologia de Materiais (DIMAT), Instituto Nacional de Metrologia, Normalização e Qualidade Industrial (INMETRO), Duque de Caxias, RJ 25250-020 (Brazil); Sousa, V.S.R. de; Caldas, A.; Oliveira, N.A. de [Instituto de Física, Universidade do Estado do Rio de Janeiro—UERJ, Rua São Francisco Xavier, 524, 20550-013 RJ (Brazil)

    2013-09-15

    One of the biggest challenges in materials science is to understand the microscopic mechanisms responsible in storage and release material entropy. TbN compound, which presents non-degeneracy in ground state, was studied and the calculated magnetocaloric effect is in good agreement with the recent experimental data. Also inverse magnetocaloric effect and spin reorientation transition were predicted in TbN. The theoretical investigations were carried out using a Hamiltonian, which includes the crystalline electrical field, Zeeman and exchange interactions. - Highlights: • Theoretical description of the magnetocaloric effect in TbN. • Influence of the crystalline electrical field anisotropy on TbN. • Predictions of inverse and anomalous magnetocaloric effect in TbN.

  15. Magnetic refrigeration at room temperature - from magnetocaloric materials to a prototype

    DEFF Research Database (Denmark)

    Kuhn, Luise Theil; Pryds, Nini; Bahl, Christian Robert Haffenden

    2011-01-01

    materials, their shaping and graded composition for technological use. Modelling the performance of a permanent magnet with optimum use of the flux and relatively low weight, and designing and constructing a prototype continuous magnetic refrigeration device have also been major tasks in the project......Based on the magnetocaloric effect, magnetic refrigeration at room temperature has for the past decade been a promising, environmentally friendly new energy technology predicted to have a significantly higher efficiency than the present conventional methods. However, so far only a few prototype...... refrigeration machines have been presented worldwide and there are still many scientific and technological challenges to be overcome. We report here on the MagCool project, which spans all the way from basic materials studies to the construction of a prototype. Emphasis has been on ceramic magnetocaloric...

  16. Properties of magnetocaloric materials with a distribution of Curie temperatures

    DEFF Research Database (Denmark)

    Bahl, Christian Robert Haffenden; Bjørk, Rasmus; Smith, Anders

    2012-01-01

    The magnetocaloric properties of inhomogeneous ferromagnets that contain distributions of Curie temperatures are considered as a function of the width of such a distribution. Assuming a normal distribution of the Curie temperature, the average adiabatic temperature change, ΔTad, the isothermal...... magnetic entropy change, Δs, and the heat capacity, cp, in zero magnetic field and an applied magnetic field of , have been calculated using the mean field model of ferromagnetism. Interestingly, both the peak position and amplitude of each of these parameters vary differently with the width...... of the distribution, explaining the observed mismatch of peak temperatures reported in experiments. Also, the field dependence of ΔTad and Δs is found to depend on the width of the distribution....

  17. Nonuniversal scaling of the magnetocaloric effect as an insight into spin-lattice interactions in manganites

    DEFF Research Database (Denmark)

    Smith, Anders; Nielsen, Kaspar Kirstein; Neves Bez, Henrique

    2016-01-01

    . In this way the determination of the nonuniversal field dependence of the magnetocaloric effect close to a phase transition can be used as a method to gain insight into the strength of the spin-lattice interactions of magnetic materials. The approach is shown also to be applicable to first-order transitions.......We measure the magnetocaloric effect of the manganite series La0.67Ca0.33-xSrxMnO3 by determining the isothermal entropy change upon magnetization, using variable-field calorimetry. The results demonstrate that the field dependence of the magnetocaloric effect close to the critical temperature...... is not given uniquely by the critical exponents of the ferromagnetic-paramagnetic phase transition, i.e., the scaling is nonuniversal. A theoretical description based on the Bean-Rodbell model and taking into account compositional inhomogeneities is shown to be able to account for the observed field dependence...

  18. Barocaloric effect in the magnetocaloric prototype Gd5Si2Ge2

    Energy Technology Data Exchange (ETDEWEB)

    Yuce, Suheyla; Barrio, Maria; Emre, Baris; Stern-Taulats, Enric; Planes, Antoni; Tamarit, Josep-Lluis; Mudryk, Yaroslav; Gschneidner, Karl A.; Pecharsky, Vitalij K.; Manosa, Lluis

    2012-08-16

    We report on calorimetric measurements under hydrostatic pressure that enabled us to determine the barocaloric effect in Gd5Si2Ge2. The values for the entropy change for moderate pressures compare favourably to those corresponding to the magnetocaloric effect in this compound. Entropy data are complemented with direct measurements of the adiabatic pressure-induced temperature change.

  19. The effect of tapering on a magnetocaloric regenerator bed

    DEFF Research Database (Denmark)

    Dallolio, Stefano; Lei, Tian; Engelbrecht, Kurt

    2017-01-01

    To design a high efficiency magnetocaloric heat pump for the residential sector, we focused on the improvement of the performance of the regenerator bed. In particular, placing the regenerators circumferentially on a plane, we decided to use tapered regenerators instead of the straight channel ones....... Therefore, this paper investigates the effect of the tapering of the regenerators, which exhibit better air-gap utilization. Several simulations using a 1D AMR model were run to study the performance of the tapered regenerator, and the results were compared to the case of the straight regenerator bed....... Moreover, the temperature span was held fixed at 25 K, and the working temperature of the regenerator was shifted to study the sensitivity to the variation of the working conditions. This paper considers a 10-layer regenerator, with Curie temperature (TC) spacing of 2.5 K....

  20. Investigation on the magnetocaloric effect in (Gd,Pr)Al{sub 2} solid solutions

    Energy Technology Data Exchange (ETDEWEB)

    Sousa, V.S.R. de, E-mail: vinidesousa@gmail.co [Instituto de Fisica ' Armando Dias Tavares' , Universidade do Estado do Rio de Janeiro, Rua Sao Francisco Xavier, 524 Maracana, Rio de Janeiro, RJ 20550-013 (Brazil); Carvalho, A. Magnus G. [Divisao de Metrologia de Materiais, Inmetro, Duque de Caxias, RJ 25250-020 (Brazil); Plaza, E.J.R. [Departamento de Fisica, Universidade Federal de Sergipe, 49100-000 Sao Cristovao, Sergipe (Brazil); Alho, B.P. [Instituto de Fisica ' Armando Dias Tavares' , Universidade do Estado do Rio de Janeiro, Rua Sao Francisco Xavier, 524 Maracana, Rio de Janeiro, RJ 20550-013 (Brazil); Tedesco, J.C.G.; Coelho, A.A. [Instituto de Fisica ' Gleb Wataghin' , Unicamp, 13083-970 Campinas, SP (Brazil); Oliveira, N.A. de; Ranke, P.J. von [Instituto de Fisica ' Armando Dias Tavares' , Universidade do Estado do Rio de Janeiro, Rua Sao Francisco Xavier, 524 Maracana, Rio de Janeiro, RJ 20550-013 (Brazil)

    2011-03-15

    A theoretical and experimental investigation on the magnetocaloric properties of the rare earth pseudo-binary compounds Gd{sub 1-n}Pr{sub n}Al{sub 2} is presented. The calculated isothermal entropy and adiabatic temperature changes under magnetic field variations from 0 to 2 T and from 0 to 5 T are in good agreement with the experimental data. For the Pr-concentrations n=0.25, 0.5 and 0.75 the experimental data present an inverse magnetocaloric effect which was theoretically predicted and associated with the competition between the opposite magnetizations of the Gd and Pr sublattices. The two-sublattice Hamiltonian used in the calculations takes into account the crystal field, exchange and Zeeman interactions. - Research highlights: > Ferrimagnetic coupling between Gd and Pr ions. > Ferrimagnetic coupling leads to an inverse magnetocaloric effect. > An inversion in the magnetization sublattices is predicted.

  1. Inverse and normal magnetocaloric effects in LaFe12B6

    International Nuclear Information System (INIS)

    Diop, L. V. B.; Isnard, O.

    2016-01-01

    Intrinsic magnetic properties and magnetocaloric effect were studied for LaFe 12 B 6 itinerant-electron system, which presents an antiferromagnetic ground state below 36 K. For certain magnetic fields values, LaFe 12 B 6 exhibits a sequence of two successive magnetic transitions: an antiferromagnetic-ferromagnetic (AFM-FM) transition at low temperature followed by a ferromagnetic-paramagnetic transition, leading to normal and inverse magnetocaloric effects, respectively. At finite temperatures, both antiferromagnetic (AFM) and paramagnetic states can be transformed into a ferromagnetic (FM) state via a field-induced metamagnetic transition accompanied with a huge magnetic hysteresis. Moreover, we reveal that, at low temperatures, the magnetization displays abrupt jumps across the first-order AFM-FM transition, giving rise to an unusual and unique staircase-like behavior. LaFe 12 B 6 exhibits both normal magnetocaloric effect around the Curie temperature and large inverse magnetocaloric effect around the AFM-FM transition temperature; for μ 0 ΔH = 7 T, ΔS M is found to be −6.8 and 19 J kg −1  K −1 around 38 and 8 K, respectively.

  2. Large magnetocaloric effect of GdNiAl2 compound

    International Nuclear Information System (INIS)

    Dembele, S.N.; Ma, Z.; Shang, Y.F.; Fu, H.; Balfour, E.A.; Hadimani, R.L.; Jiles, D.C.; Teng, B.H.; Luo, Y.

    2015-01-01

    This paper presents the structure, magnetic properties, and magnetocaloric effect of the polycrystalline compound GdNiAl 2 . Powder X-ray diffraction (XRD) measurement and Rietveld refinement revealed that GdNiAl 2 alloy is CuMgAl 2 -type phase structure with about 1 wt% GdNi 2 Al 3 secondary phase. Magnetic measurements suggest that the compound is ferromagnetic and undergoes a second-order phase transition near 28 K. The maximum value of magnetic entropy change reaches 16.0 J/kg K for an applied magnetic field change of 0–50 kOe and the relative cooling power was 6.4×10 2 J/kg. It is a promising candidate as a magnetocaloric material working near liquid hydrogen temperature (~20 K) exhibiting large relative cooling power. - Highlights: • Preferred orientation with axis of [010] was found in the GdNiAl 2 compound. • The ΔS Mmax and the RCP are 16.0 J/kg K and 640 J/kg, respectively, for ΔH=50 kOe. • Relative low rare earth content in GdNiAl 2 comparing with other candidates

  3. The effect of plastic deformation on magnetic and magnetocaloric properties of Gd-B alloys

    Science.gov (United States)

    Taskaev, Sergey; Skokov, Konstantin; Karpenkov, Dmitry; Khovaylo, Vladimir; Ulyanov, Maxim; Bataev, Dmitry; Dyakonov, Alexandr; Fazlitdinova, Alfiya; Gutfleisch, Oliver

    2017-11-01

    We report on the magnetocaloric effect in Gd100-xBx (x = 0, 10, 15) cold rolled ribbons. A moderate entropy change ΔS = 5 J/kg·K and adiabatic change of ΔT = 4.8 K were observed for the as-cast materials in an external magnetic field of 3 T which is less by 20% in comparison with the pure gadolinium metal. It was found that a significant (up to 70%) depression of magnetization and magnetocaloric properties developed in the course of plastic deformation can completely be restored by means of a high temperature heat treatment. It is concluded that cold rolling is one promising technique for producing foil shaped magnetocaloric materials suitable for designing heat exchangers of magnetic cooling devices.

  4. Magnetic hysterysis evolution of Ni-Al alloy with Fe and Mn substitution by vacuum arc melting to produce the room temperature magnetocaloric effect material

    Energy Technology Data Exchange (ETDEWEB)

    Notonegoro, Hamdan Akbar [PPS Materials Science, FMIPA-Universitas Indonesia, Depok 16424 (Indonesia); Mechanical Engineering Dept., FT-Universitas Sultan Ageng Tirtayasa, Cilegon 42435 (Indonesia); Kurniawan, Budhy; Manaf, Azwar, E-mail: azwar@sci.ui.ac.id [PPS Materials Science, FMIPA-Universitas Indonesia, Depok 16424 (Indonesia); Setiawan, Jan [Center for Nuclear Fuel Tecnology-Badan Tenaga Atom Nasional, Tangerang Selatan 15310 (Indonesia)

    2016-06-17

    The development of magnetocaloric effect (MCE) material is done in order to reduce the damage of the ozone layer caused by the chlorofluorocarbons (CFCs) emitted into the air. The research dealing with synthesis of magnetocaloric materials based of Ni-Al Heusler Alloy structure and by varying substitution some atoms of Ni with Fe and Al with Mn on Ni-Al Heusler Alloy structure to become Ni{sub 44}Fe{sub 6}Mn{sub 32}Al{sub 18}. Vacuum Arc Melting (VAM) equipment is used to form the alloys on vacuum condition and by flowing argon gas atmosphere and then followed by annealing process for 72 hours. X-Ray Diffraction (XRD) reveals that crystallite structure of material is observed. We define that Ni{sub 44}Fe{sub 6} as X{sub 2}, Mn{sub 25} as Y, and Al{sub 18}Mn{sub 7} as Z. Based on the XRD result, we observed that the general formula X{sub 2}YZ is not changed. The PERMAGRAF measurement revealed that there exists of magnetic hysterysis. The hysterysis show that the magnetic structures of the system undego evolution from diamagnetic to soft ferromagnetic material which all of the compound have the same crystallite structure. This evolution indicated that the change in the composition has led to changes the magnetic composition. Mn is the major element that gives strong magnetic properties to the sample. When Mn partially replaced position of Al, the sample became dominant to be influenced to improve their magnetic properties. In addition, substitution a part of Ni by Fe in the composition reveals a pinning of the domain walls in the sample.

  5. Experimental results for a magnetic refrigerator using three different types of magnetocaloric material regenerators

    DEFF Research Database (Denmark)

    Engelbrecht, Kurt; Bahl, Christian Robert Haffenden; Nielsen, Kaspar Kirstein

    2011-01-01

    refrigeration device for near room temperature applications, and it is driven by the magnetocaloric effect in the regenerator material. Several magnetocaloric materials with potential magnetic refrigeration applications have recently been developed and characterized; however, few of them have been tested...

  6. Magnetocaloric materials

    Energy Technology Data Exchange (ETDEWEB)

    Jeppesen, Stinus

    2008-10-15

    New and improved magnetocaloric materials are one of the cornerstones in the development of room temperature magnetic refrigeration. Magnetic refrigeration has been used since the 1930ies in cryogenic applications, but has since the discovery of room temperature refrigerants received enormous attention. This Ph.D. work has been mainly concerned with developing a new technique to characterize the magnetocaloric effect (MCE) and using this technique in the investigations on new and improved magnetocaloric materials. For this purpose a novel differential scanning calorimeter (DSC) with applied magnetic fields was developed for measuring heat capacity as function of magnetic field. Measurements using the developed DSC demonstrate a very high sensitivity, fast measurements and good agreement with results obtained by other techniques. Furthermore, two material systems have been described in this work. Both systems take basis in the mixed-valence manganite system La{sub 1-x}Ca{sub x}MnO{sub 3} well known from research on colossal magnetoresistance (CMR). The mixed-valence manganite crystallizes in the perovskite structure of general formula ABO{sub 3}. The first material system is designed to investigate the influence of low level Cu doping on the B-site. Six different samples were prepared with over-stoichiometric compositions La{sub 0.67}Ca{sub 0.33}Mn{sub 1.05}Cu{sub x}O{sub 3}, x=0, 1, 2, 3, 4 and 5%. All compositions crystallized well in the same perovskite structure, but the morphology of the samples changed drastically with doping. Investigation on the magnetocaloric properties revealed that small levels of Cu up to around 3% could improve the magnetocaloric performance of the materials. Furthermore, Cu could be used to tune the temperature interval without deteriorating the MCE, which is a much desired characteristic for potential use in magnetic refrigerators. A less comprehensive part of the work has been concerned with the investigation of doping on the A

  7. Metamagnetism, sign reversal and low temperature magnetocaloric effect in single-crystalline EuV2Al20

    Science.gov (United States)

    Ramesh Kumar, K.; Nair, Harikrishnan S.; Bhattacharyya, A.; Thamizhavel, A.; Strydom, André M.

    2018-04-01

    The Frank-Kasper cage compound EuV2Al20 crystallizes in the cubic structure with Fd 3 ‾ m space group and exhibits unusual magnetic and transport properties. The system undergoes an antiferromagnetic transition below 5.6 K wherein the Eu2+ moments are aligned anti-parallel along 〈1 1 1〉 direction and the system exhibits a weak metamagetic transition at the field of 1 T. Arrott plots (M2 vs H / M) show a "S" shaped variation in the low fields below TN and the plausible reason for the occurrence of negative slope is discussed. Isothermal magnetic entropy change is estimated from both magnetization and heat capacity measurements invoking the Maxwell's thermodynamic relations. Temperature variation of ΔSm showed a weak negative minimum and a sign reversal at the field value of 1 T due to field induced metamagnetic transition. Universal master curve is constructed by rescaling the ΔSm vs T curves in the context of analysing the nature of the magnetic transition.

  8. Review of magnetocaloric effect in perovskite-type oxides

    International Nuclear Information System (INIS)

    Zhong Wei; Du You-Wei; Au Chak-Tong

    2013-01-01

    We survey the magnetocaloric effect in perovskite-type oxides (including doped ABO 3 -type manganese oxides, A 3 B 2 O 7 -type two-layered perovskite oxides, and A 2 B'B″O 6 -type ordered double-perovskite oxides). Magnetic entropy changes larger than those of gadolinium can be observed in polycrystalline La 1−x Ca x MnO 3 and alkali-metal (Na or K) doped La 0.8 Ca 0.2 MnO 3 perovskite-type manganese oxides. The large magnetic entropy change produced by an abrupt reduction of magnetization is attributed to the anomalous thermal expansion at the Curie temperature. Considerable magnetic entropy changes can also be observed in two-layered perovskites La 1.6 Ca 1.4 Mn 2 O 7 and La 2.5−x K 0.5+x Mn 2 O 7+δ (0 2 Fe 1+X Mo 1−x O 6 (0 ≤ x ≤ 0.3) near their respective Curie temperatures. Compared with rare earth metals and their alloys, the perovskite-type oxides are lower in cost, and they exhibit higher chemical stability and higher electrical resistivity, which together favor lower eddy-current heating. They are potential magnetic refrigerants at high temperatures, especially near room temperature. (topical review - magnetism, magnetic materials, and interdisciplinary research)

  9. Magnetocaloric effect in rare-earth intermetallics: Recent trends

    Indian Academy of Sciences (India)

    the magnetism. The giant magnetocaloric material Gd5Si2Ge2 and the related Gd5(Si, Ge)4 phases are considered the next best candidates (table 1) [2,3,25]. The variation in Si:Ge ratio in these compounds yields a wide tunability in magnetic transition temperature (from. ∼20 K to ∼280 K) retaining the giant MCE through ...

  10. The influence of the magnetoelastic interaction on the magnetocaloric effect in ferrimagnetic systems: a theoretical investigation

    Energy Technology Data Exchange (ETDEWEB)

    Alho, B P; De Oliveira, N A; De Sousa, V S R; Von Ranke, P J [Instituto de Fisica ' Armando Dias Tavares' , Universidade do Estado do Rio de Janeiro-UERJ, Rua Sao Francisco Xavier 524, 20550-013, RJ (Brazil); Plaza, E J R [Departamento de Fisica, Universidade Federal de Sergipe, 49100-000, Sao Cristovao, Sergipe (Brazil); Magnus G Carvalho, A, E-mail: brunoalho@gmail.co [Divisao de Metrologia de Materiais, Instituto Nacional de Metrologia, Normalizacao e Qualidade Industrial (INMETRO), 25250-020, Duque de Caxias, RJ (Brazil)

    2010-12-08

    In this work the magnetocaloric effect is theoretically investigated considering a microscopic model Hamiltonian, which describes a magnetic system formed by two sublattices of different magnetic ions coupled by exchange and magnetoelastic interactions. We analyze systematically several profiles of the ferrimagnetic arrangements that were studied earlier without the magnetoelastic interaction. The influence of changing the magnetoelastic parameters on the magnetization, isothermal entropy change and adiabatic temperature change curves are investigated. Depending on the model parameters, the magnetic system shows a first-order magnetic phase transition leading to high direct and inverse magnetocaloric effect, besides two simultaneous first-order magnetic phase transitions which were predicted. A constant {Delta}S{sub T} = 0.4 J mol{sup -1} K{sup -1} is obtained in the simulated system in a temperature interval of 50 K, around 110 K.

  11. Study of magnetocaloric effect in LaFe11∙ 5Si1∙ 5 alloys prepared by ...

    Indian Academy of Sciences (India)

    For studying the influence of different cooling processes on magnetic properties, the Curie temperature, thermal and magnetic hysteresis, magnetocaloric effect and relative cooling power are investigated. The result shows that the Curie temperature of LaFe11.5Si1.5 prepared by quenching in ice water is 197.6 K, about 4 K ...

  12. Colossal magnetocaloric effect in magneto-auxetic systems

    Science.gov (United States)

    Dudek, M. R.; Wojciechowski, K. W.; Grima, J. N.; Caruana-Gauci, R.; Dudek, K. K.

    2015-08-01

    We show that a mechanically driven magnetocaloric effect (MCE) in magneto-auxetic systems (MASs) in the vicinity of room temperature is possible and the effect can be colossal. Even at zero external magnetic field, the magnetic entropy change in this reversible process can be a few times larger in magnitude than in the case of the giant MCE discovered by Pecharsky and Gschneidner in Gd5(Si2Ge2). MAS represent a novel class of metamaterials having magnetic insertions embedded within a non-magnetic matrix which exhibits a negative Poisson’s ratio. The auxetic behaviour of the non-magnetic matrix may either enhance the magnetic ordering process or it may result in a transition to the disordered phase. In the MAS under consideration, a spin 1/2 system is chosen for the magnetic component and the well-known Onsager solution for the two-dimensional square lattice Ising model at zero external magnetic field is used to show that the isothermal change in magnetic entropy accompanying the auxetic behaviour can take a large value at room temperature. The practical importance of our findings is that MCE materials used in present engineering applications may be further enhanced by changing their geometry such that they exhibit auxetic behaviour.

  13. Colossal magnetocaloric effect in magneto-auxetic systems

    International Nuclear Information System (INIS)

    Dudek, M R; Dudek, K K; Wojciechowski, K W; Grima, J N; Caruana-Gauci, R

    2015-01-01

    We show that a mechanically driven magnetocaloric effect (MCE) in magneto-auxetic systems (MASs) in the vicinity of room temperature is possible and the effect can be colossal. Even at zero external magnetic field, the magnetic entropy change in this reversible process can be a few times larger in magnitude than in the case of the giant MCE discovered by Pecharsky and Gschneidner in Gd 5 (Si 2 Ge 2 ). MAS represent a novel class of metamaterials having magnetic insertions embedded within a non-magnetic matrix which exhibits a negative Poisson’s ratio. The auxetic behaviour of the non-magnetic matrix may either enhance the magnetic ordering process or it may result in a transition to the disordered phase. In the MAS under consideration, a spin 1/2 system is chosen for the magnetic component and the well-known Onsager solution for the two-dimensional square lattice Ising model at zero external magnetic field is used to show that the isothermal change in magnetic entropy accompanying the auxetic behaviour can take a large value at room temperature. The practical importance of our findings is that MCE materials used in present engineering applications may be further enhanced by changing their geometry such that they exhibit auxetic behaviour. (paper)

  14. Magnetocaloric effect in Sr2FeMoO6/Ag composites

    Directory of Open Access Journals (Sweden)

    Mahmoud A. Hamad

    2015-03-01

    Full Text Available The enhanced low-field magnetocaloric effect was investigated for double perovskite Sr2FeMoO6 - silver (SFMO/Ag composites with 0, 5 and 10 wt.% of Ag. A phenomenological model was used to predict magnetocaloric properties of SFMO/Ag composites, such as magnetic entropy change, heat capacity change and relative cooling power. It was shown that magnetic entropy change (∆S M peaks of SFMO/Ag span over a wide temperature region, which can significantly improve the global efficiency of the magnetic refrigeration. Furthermore, the ∆S M distribution of the SFMO/Ag composites is much more uniform than that of gadolinium. Through these results, SFMO/Ag composite has some potential application for magnetic refrigerants in an extended high-temperature range.

  15. Observation of large magnetocaloric effect in equiatomic binary compound ErZn

    Directory of Open Access Journals (Sweden)

    Lingwei Li

    2017-05-01

    Full Text Available The magnetism, magnetocaloric effect and universal behaviour in rare earth Zinc binary compound of ErZn have been studied. The ErZn compound undergoes a second order paramagnetic (PM to ferromagnetic (FM transition at Curie temperature of TC ∼ 20 K. The ErZn compound exhibits a large reversible magnetocaloric effect (MCE around its own TC. The rescaled magnetic entropy change curves overlap with each other under various magnetic field changes, further confirming the ErZn with the second order phase transition. For the magnetic field change of 0-7 T, the maximum values of the magnetic entropy change (−ΔSMmax, relative cooling power (RCP and refrigerant capacity (RC for ErZn are 23.3 J/kg K, 581 J/kg and 437 J/kg, respectively.

  16. Magnetocaloric effect in “reduced” dimensions: Thin films, ribbons, and microwires of Heusler alloys and related compounds: Magnetocaloric effect in “reduced” dimensions

    Energy Technology Data Exchange (ETDEWEB)

    Khovaylo, Vladimir V. [National University of Science and Technology MISiS, Moscow 119049 Russia; ITMO University, St. Petersburg 197101 Russia; Rodionova, Valeria V. [National University of Science and Technology MISiS, Moscow 119049 Russia; Innovation Park and Institute of Physics & Technology, Immanuel Kant Baltic Federal University, Kaliningrad 236041 Russia; Shevyrtalov, Sergey N. [Innovation Park and Institute of Physics & Technology, Immanuel Kant Baltic Federal University, Kaliningrad 236041 Russia; Novosad, Val [Materials Science Division, Argonne National Laboratory, Argonne IL 60439 USA

    2014-08-19

    Room temperature magnetic refrigeration is an energy saving and environmentally-friendly technology which has developed rapidly from a basic idea to prototype devices. The performance of magnetic refrigerators crucially depends on the magnetocaloric properties and the geometry of the employed refrigerants. Here we review the magnetocaloric properties of Heusler alloys and related compounds with a high surface to volume ratio such as films, ribbons and microwires, and compare them with their bulk counterparts.

  17. Magnetocaloric Materials and the Optimization of Cooling Power Density

    Science.gov (United States)

    Wikus, Patrick; Canavan, Edgar; Heine, Sarah Trowbridge; Matsumoto, Koichi; Numazawa, Takenori

    2014-01-01

    The magnetocaloric effect is the thermal response of a material to an external magnetic field. This manuscript focuses on the physics and the properties of materials which are commonly used for magnetic refrigeration at cryogenic temperatures. After a brief overview of the magnetocaloric effect and associated thermodynamics, typical requirements on refrigerants are discussed from a standpoint of cooling power density optimization. Finally, a compilation of the most important properties of several common magnetocaloric materials is presented.

  18. Near room temperature magnetocaloric properties and the universal curve of MnCoGe1-xCux

    Science.gov (United States)

    Si, Xiaodong; Liu, Yongsheng; Lu, Xiaofei; Shen, Yulong; Wang, Wenli; Yu, Wenying; Zhou, Tao; Gao, Tian

    2017-05-01

    Intermetallic compounds based on MnCoGe have drawn attention due to the coupled magnetic and structural transformations and the large magnetocaloric entropy. Here, we provide a systematic comparison of experimental data under different magnetic fields with magnetic and the magnetocaloric properties. The ferromagnetic transition temperature (TC) increases from 353.4(6) K for x = 0.01 to 363.4(4) K for x = 0.04 with increasing nominal copper content. The maximum magnetic entropy change |ΔSM| in a magnetic field change of 5 T is found to be 18.3(2) J/(kg K) with a large relative cooling power (RCP) value of 292.5(4) J/kg for x = 0.01, revealing that the present system can provide an acceptable magnetocaloric effect at a cheaper price for magnetic refrigeration materials. Making attempt to contrast a master curve for the present system, we find the experimental values of magnetic field dependence of the magnetic entropy change are consistent with a phenomenological universal curve.

  19. The influence of magnetic and electric coupling properties on the magnetocaloric effect in quantum paraelectric EuTiO{sub 3}

    Energy Technology Data Exchange (ETDEWEB)

    Ranke, P.J. von, E-mail: von.ranke@uol.com.br [Instituto de Fisica, Universidade do Estado do Rio de Janeiro-UERJ, Rua Sao Francisco Xavier, 524, 20550-013 RJ (Brazil); Alho, B.P.; Nobrega, E.P. [Instituto de Fisica, Universidade do Estado do Rio de Janeiro-UERJ, Rua Sao Francisco Xavier, 524, 20550-013 RJ (Brazil); Sousa, V.S.R. de [Instituto de Fisica Gleb Wataghin, Universidade Estadual de Campinas-UNICAMP, 13083-970 Campinas, SP (Brazil); Alvarenga, T.S.T. [Instituto de Fisica, Universidade do Estado do Rio de Janeiro-UERJ, Rua Sao Francisco Xavier, 524, 20550-013 RJ (Brazil); Carvalho, A. Magnus G. [Divisao de Metrologia de Materiais (DIMAT), Instituto Nacional de Metrologia, Normalizacao e Qualidade Industrial (INMETRO), Duque de Caxias, RJ 25250-020 (Brazil); Oliveira, N.A. de [Instituto de Fisica, Universidade do Estado do Rio de Janeiro-UERJ, Rua Sao Francisco Xavier, 524, 20550-013 RJ (Brazil)

    2012-04-15

    We report on the magnetic and magnetocaloric effect calculations in antiferromagnetic perovskite-type EuTiO{sub 3}. From the isothermal magnetic entropy change calculated upon low magnetic field changes (below 1 T) several results were predicted: inverse magnetocaloric effect, latent heat associated to spin AFM-FM reorientation transition and a temperature interval (controlled by magnetic field) where the EuTiO{sub 3} does not change heat in an isothermic process. The magnetocaloric effect described through magnetic entropy change was correlated with magnetocapacitance formula. The theoretical investigation was carried out using a Heisenberg Hamiltonian considering the G-type antiferromagnetic structure with exchange interactions, in mean field approximation, between nearest-neighbor and next-nearest-neighbor magnetic Eu{sup +2} ions. - Highlights: Black-Right-Pointing-Pointer We model the quantum paraelectric EuTiO{sub 3} compound and the magnetocaloric effect was investigated. Black-Right-Pointing-Pointer Inverse magnetocaloric effect and the latent heat associated to the spin reorientation transition were predicted. Black-Right-Pointing-Pointer The magnetocaloric and dielectric properties in EuTiO{sub 3} were correlated.

  20. Pressure effect on phase transitions and magnetocaloric effect in Gd.sub.5./sub.Ge.sub.4./sub..

    Czech Academy of Sciences Publication Activity Database

    Arnold, Zdeněk; Skorokhod, Yuriy; Kamarád, Jiří; Magen, C.; Algarabel, P.A.

    2009-01-01

    Roč. 105, č. 3 (2009), 07A934/1-07A934/3 ISSN 0021-8979 R&D Projects: GA ČR(CZ) GA106/06/0368 Institutional research plan: CEZ:AV0Z10100521 Keywords : Curie temperature * ferromagnetic materials * ferromagnetic-antiferromagnetic transitions * gadolinium compounds * magnetocaloric effect Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 2.072, year: 2009

  1. Hysteresis in Magnetocaloric Materials

    DEFF Research Database (Denmark)

    von Moos, Lars

    In this thesis the effects of hysteresis on magnetocaloric material properties and their performance in magnetic refrigeration devices are investigated. This is done through an experimental and model study of first order magnetocaloric materials MnFe(P,As) and Gd5Si2Ge2. The experimental characte......In this thesis the effects of hysteresis on magnetocaloric material properties and their performance in magnetic refrigeration devices are investigated. This is done through an experimental and model study of first order magnetocaloric materials MnFe(P,As) and Gd5Si2Ge2. The experimental...... cases. The Gd5Si2Ge2 model is based on detailed first order reversal curve data, taking both reversible and irreversible properties into account, and is able to reproduce a series of independent experimental results. The Preisach models are applied to simulate material behavior under realistic...... set points, which is demonstrated to induce partial hysteresis loop behavior that will generally underestimate thermal hysteresis. Furthermore it is shown that care should be taken in non-isofield type experiments, as is the case for direct MCE experiments. Measuring the temperature dependence...

  2. Monte Carlo simulation study of magnetocaloric effect in NdMnO{sub 3} perovskite

    Energy Technology Data Exchange (ETDEWEB)

    Masrour, R., E-mail: rachidmasrour@hotmail.com [Laboratory of Materials, Processes, Environment and Quality, Cady Ayyed University, National School of Applied Sciences, PB 63 46000 Safi (Morocco); Laboratoire de Magnétisme et Physique des Hautes Energies L.M.P.H.E.URAC 12, Université Mohammed V, Faculté des Sciences, B.P. 1014, Rabat (Morocco); Jabar, A. [Laboratoire de Magnétisme et Physique des Hautes Energies L.M.P.H.E.URAC 12, Université Mohammed V, Faculté des Sciences, B.P. 1014, Rabat (Morocco); Benyoussef, A. [Laboratoire de Magnétisme et Physique des Hautes Energies L.M.P.H.E.URAC 12, Université Mohammed V, Faculté des Sciences, B.P. 1014, Rabat (Morocco); Institute of Nanomaterials and Nanotechnologies, MAScIR, Rabat (Morocco); Hassan II Academy of Science and Technology, Rabat (Morocco); Hamedoun, M. [Institute of Nanomaterials and Nanotechnologies, MAScIR, Rabat (Morocco); Hlil, E.K. [Institut Curie, CNRS et Université Joseph Fourier, BP 166, F-38042 Grenoble Cedex 9 (France)

    2016-03-01

    The magnetocaloric effect in NdMnO{sub 3} perovskite is investigated by using the Monte Carlo simulations. The Curie temperature T{sub C} of NdMnO{sub 3} compound is deduced from the variation of the magnetization vs. the temperature with different values of external magnetic field. The variation of magnetization with the external magnetic field H is given. The specific heat with the temperature is established for different external magnetic field. The thermal magnetic entropy for different external magnetic field and different exchange interactions in NdMnO{sub 3} compound is obtained. The adiabatic temperature change is obtained. The relative cooling power with different external magnetic field is established. The magnetocaloric effect has been investigated from magnetization. - Highlights: • Results obtained show that the PM–FM transition is of second order in NdMnO{sub 3}. • Critical properties of NdSi at the FM–PM transition have been analyzed. • The Curie temperature and magnetic entropy have been obtained.

  3. Adiabatic measurements of magneto-caloric effects in pulsed high magnetic fields up to 55 T

    Science.gov (United States)

    Kihara, T.; Kohama, Y.; Hashimoto, Y.; Katsumoto, S.; Tokunaga, M.

    2013-07-01

    Magneto-caloric effects (MCEs) measurement system in adiabatic condition is proposed to investigate the thermodynamic properties in pulsed magnetic fields up to 55 T. With taking the advantage of the fast field-sweep rate in pulsed field, adiabatic measurements of MCEs were carried out at various temperatures. To obtain the prompt response of the thermometer in the pulsed field, a thin film thermometer is grown directly on the sample surfaces. The validity of the present setup was demonstrated in the wide temperature range through the measurements on Gd at about room temperature and on Gd3Ga5O12 at low temperatures. The both results show reasonable agreement with the data reported earlier. By comparing the MCE data with the specific heat data, we could estimate the entropy as functions of magnetic field and temperature. The results demonstrate the possibility that our approach can trace the change in transition temperature caused by the external field.

  4. Theoretical investigations on the magnetocaloric and barocaloric effects in Tb{sub y}Gd{sub (1−y)}Al{sub 2} series

    Energy Technology Data Exchange (ETDEWEB)

    Ribeiro, P.O.; Alho, B.P.; Alvarenga, T.S.T.; Nóbrega, E.P. [Instituto de Física, Universidade do Estado do Rio de Janeiro – UERJ, Rua São Francisco Xavier, 524, 20550-013 RJ (Brazil); Carvalho, A.Magnus G. [Instituto de Ciência e Tecnologia, Universidade Federal de São Paulo – UNIFESP, 12231-280 São José dos Campos, SP (Brazil); Instituto Nacional de Metrologia, Qualidade e Tecnologia – INMETRO, 25250-020 Duque de Caxias, RJ (Brazil); Sousa, V.S.R. de; Caldas, A.; Oliveira, N.A. de [Instituto de Física, Universidade do Estado do Rio de Janeiro – UERJ, Rua São Francisco Xavier, 524, 20550-013 RJ (Brazil); Ranke, P.J. von, E-mail: von.ranke@uol.com.br [Instituto de Física, Universidade do Estado do Rio de Janeiro – UERJ, Rua São Francisco Xavier, 524, 20550-013 RJ (Brazil)

    2013-06-25

    Highlights: ► Anisotropic magnetocaloric effect in in Tb{sub 0.4}Gd{sub 0.6}Al{sub 2}. ► Prediction of barocaloric effect in Tb{sub 0.4}Gd{sub 0.6}Al{sub 2}. ►An optimal hybrid magnetocaloric material using Tb{sub y}Gd{sub (1-y)}Al{sub 2} compounds. -- Abstract: We report the calculations on the magnetocaloric and barocaloric effects in ferromagnetic series Tb{sub y}Gd{sub (1−y)}Al{sub 2}. Our model includes the crystalline electrical field interaction, exchange interactions among Tb–Tb, Gd–Gd and Tb–Gd magnetic ions and the Zeeman effect for an anisotropic system. The lattice and electronic entropies were included in adiabatic processes. The magnetocaloric effect calculated for magnetic field changes along the easy magnetic direction 〈1 1 1〉 is in good agreement with the experimental data. Calculation along the hard magnetization direction 〈0 0 1〉 predicts anomalous magnetocaloric effect, which was ascribed to the spin reorientation processes. From the available experimental data of Curie temperature dependence on pressure, the exchange model parameters were scaled and the barocaloric effect was calculated.

  5. Magnetocaloric effect in magnetothermally-responsive nanocarriers for hyperthermia-triggered drug release

    International Nuclear Information System (INIS)

    Li Jianbo; Qu Yang; Ren Jie; Yuan Weizhong; Shi Donglu

    2012-01-01

    The magnetocaloric effects and lower critical solution temperature (LCST) were investigated in a magnetothermally-responsive nanocarrier for magnetothermal drug release under alternating magnetic field (AMF). The Mn 0.2 Zn 0.8 Fe 2 O 4 nanoparticles with low T c were dispersed in a polymeric matrix consisting of N-Isopropyl acrylamide (NIPAAm) and N-hydroxymethyl acrylamide (HMAAm). The magnetocaloric effects and LCST of the nanocarriers were characterized by using high-resolution electron transmission microscopy, thermogravimetric analyses, and vibrating sample magnetometer. The maximum self-heating temperature of 42.9 °C was achieved by optimizing the Mn 0.2 Zn 0.8 Fe 2 O 4 concentration in the polymer matrix. By adjusting the NIPAAm to HMAAm ratio, the LCST was controlled at an ideal level of 40.1 °C for efficient thermosensitive drug delivery. Magnetothermally responsive drug release of Doxorubicin, an anticancer drug, was significantly enhanced by application of an external AMF on the nanocarriers. The cytotoxicity experimental results in vitro show good biocompatibility and efficient therapeutic effects in cancer treatment. (paper)

  6. The normal and inverse magnetocaloric effect in RCu2 (R=Tb, Dy, Ho, Er) compounds

    International Nuclear Information System (INIS)

    Zheng, X.Q.; Xu, Z.Y.; Zhang, B.; Hu, F.X.; Shen, B.G.

    2017-01-01

    Orthorhombic polycrystalline RCu 2 (R=Tb, Dy, Ho and Er) compounds were synthesized and the magnetic properties and magnetocaloric effect (MCE) were investigated in detail. All of the RCu 2 compounds are antiferromagnetic (AFM) ordered. As temperature increases, RCu 2 compounds undergo an AFM to AFM transition at T t and an AFM to paramagnetic (PM) transition at T N . Besides of the normal MCE around T N , large inverse MCE around T t was found in TbCu 2 compound. Under a field change of 0–7 T, the maximal value of inverse MCE is even larger than the value of normal MCE around T N for TbCu 2 compound. Considering of the normal and inverse MCE, TbCu 2 shows the largest refrigerant capacity among the RCu 2 (R=Tb, Dy, Ho and Er) compounds indicating its potential applications in low temperature multistage refrigeration. - Highlights: • Large inverse magnetocaloric effect is observed in TbCu 2 compound. • The AFM to AFM transition is observed in RCu 2 (R=Tb, Dy, Ho, Er) compounds. • The MCE performance of TbCu 2 compound is evaluated in a more comprehensively way.

  7. Analysis of the Magnetocaloric Effect in Powder Samples Obtained by Ball Milling

    Science.gov (United States)

    Blázquez, J. S.; Ipus, J. J.; Moreno-Ramírez, L. M.; Borrego, J. M.; Lozano-Pérez, S.; Franco, V.; Conde, C. F.; Conde, A.

    2015-06-01

    Since the discovery of the giant magnetocaloric effect (MCE) close to room temperature in FeRh and particularly in Gd5Si2Ge2 compounds, the study of this phenomenon has experienced an exponential growth. Among the different techniques used to produce magnetocaloric materials, ball milling has been shown as a very versatile one and presents several advantages over other preparation techniques ( e.g., easy scale-up to industrial production). Although a general decrease of the peak value of the magnetic entropy change is observed for milled samples, it can be compensated by the large broadening of the MCE peak, leading to an increase of the refrigeration capacity. In this short review, several aspects inherent to powder samples affecting MCE will be discussed, such as the relevant effect of the demagnetizing field, the possible multiphase character, and the presence of Curie temperature distributions. In mechanically alloyed samples, the two latter factors are typically affected by the degree of integration of the different starting constituents.

  8. Analysis of the Anisotropic Magnetocaloric Effect in RMn2O5 Single Crystals

    Directory of Open Access Journals (Sweden)

    Mohamed Balli

    2017-11-01

    Full Text Available Thanks to the strong magnetic anisotropy shown by the multiferroic RMn2O5 (R = magnetic rare earth compounds, a large adiabatic temperature change can be induced (around 10 K by rotating them in constant magnetic fields instead of the standard magnetization-demagnetization method. Particularly, the TbMn2O5 single crystal reveals a giant rotating magnetocaloric effect (RMCE under relatively low constant magnetic fields reachable by permanent magnets. On the other hand, the nature of R3+ ions strongly affects their RMCEs. For example, the maximum rotating adiabatic temperature change exhibited by TbMn2O5 is more than five times larger than that presented by HoMn2O5 in a constant magnetic field of 2 T. In this paper, we mainly focus on the physics behind the RMCE shown by RMn2O5 multiferroics. We particularly demonstrate that the rare earth size could play a crucial role in determining the magnetic order, and accordingly, the rotating magnetocaloric properties of RMn2O5 compounds through the modulation of exchange interactions via lattice distortions. This is a scenario that seems to be supported by Raman scattering measurements.

  9. Spatially resolved measurements of the magnetocaloric effect and the local magnetic field using thermography

    DEFF Research Database (Denmark)

    Christensen, Dennis; Bjørk, Rasmus; Nielsen, Kaspar Kirstein

    2010-01-01

    The magnetocaloric effect causes a magnetic material to change temperature upon application of a magnetic field. Here, spatially resolved measurements of the adiabatic temperature change are performed on a plate of gadolinium using thermography. The adiabatic temperature change is used to extract...

  10. The magnetocaloric effect at the first-order magneto-elastic phase transition

    International Nuclear Information System (INIS)

    Basso, Vittorio

    2011-01-01

    This paper presents a study of the magnetocaloric effect at the first-order magneto-elastic phase transition. The entropy change Δs at the transition temperature is given by the sum of the magnetic and the structural contributions. By using a thermodynamic model, it is shown that the sign and amplitude of the structural contribution to Δs are determined by the dimensionless parameter ζ (zeta) which depends on β, the steepness of the change of exchange forces with volume, and on α p , the thermal expansion coefficient of the structural lattice. For ζ 1 the structural entropy dominates and a transition occurs upon heating from a low temperature paramagnet to a high temperature ferromagnet.

  11. The magnetocaloric effect at the first-order magneto-elastic phase transition.

    Science.gov (United States)

    Basso, Vittorio

    2011-06-08

    This paper presents a study of the magnetocaloric effect at the first-order magneto-elastic phase transition. The entropy change Δs at the transition temperature is given by the sum of the magnetic and the structural contributions. By using a thermodynamic model, it is shown that the sign and amplitude of the structural contribution to Δs are determined by the dimensionless parameter ζ (zeta) which depends on β, the steepness of the change of exchange forces with volume, and on α(p), the thermal expansion coefficient of the structural lattice. For ζ 1 the structural entropy dominates and a transition occurs upon heating from a low temperature paramagnet to a high temperature ferromagnet.

  12. Evaluation of the magnetocaloric effect from magnetization and heat capacity data

    Energy Technology Data Exchange (ETDEWEB)

    Lee, J.S. [Dept. of Precision Mechanical Engineering, Kangnung National University, Gangneung, Gangwon Province, 210-702 (Korea)

    2004-06-01

    Magnetic refrigeration is based on the magnetocaloric effect (MCE) - the ability of some materials to heat up when magnetized and cool down when removed from the magnetic field. The available techniques for studying the MCE are: (i) direct measurements by monitoring the change in material's temperature during the application or removal of the magnetic field; and (ii) indirect calculations from experimental data of magnetization and/or heat capacity as functions of temperature and magnetic field. In this paper the procedure to evaluate the MCE from magnetization and zero-field heat capacity data is described. The MCE - isothermal magnetic entropy change ({delta}S{sub M}) and adiabatic temperature change ({delta}T{sub ad}) - of gadolinium (Gd) obtained by this procedure is presented. (copyright 2004 WILEY-VCH Verlag GmbH and Co. KGaA, Weinheim) (orig.)

  13. Magnetization and Magnetocaloric Effect in Sol-Gel Derived Nanocrystalline Copper-Zinc Ferrite.

    Science.gov (United States)

    Anwar, M S; Ahmed, Faheem; Koo, Bon Heun

    2015-02-01

    We report the sol-gel synthesis and magnetocaloric effect in nanocrystalline copper-zinc ferrite (Cu0.5Zn0.5Fe2O4). The synthesized powder was characterized by using X-ray diffraction (XRD), field emission scanning electron microscopy (FE-SEM), energy dispersive X-ray spectroscopy (EDX) and magnetization measurements. The XRD results confirm the formation of single phase spinel structure. The average particle size was found to be ~58 nm. FE-SEM results suggested that the nanoparticles are agglomerated and spherical in shape. Magnetization measurement reveals that Cu0.5Zn0.5Fe2O4 nanoparticles exhibit transition temperature (Tc) above room temperature. The maximum magnetic entropy change (ΔSM)max shows interesting behaviour and was found to vary with the applied magnetic field. This nanopowder can be considered as potential material for magnetic refrigeration above room temperature.

  14. Large magnetocaloric effect of GdNiAl{sub 2} compound

    Energy Technology Data Exchange (ETDEWEB)

    Dembele, S.N.; Ma, Z.; Shang, Y.F. [School of Physical Electronics, University of Electronic Science and Technology of China, Chengdu 610054 (China); Fu, H., E-mail: fuhao@uestc.edu.cn [School of Physical Electronics, University of Electronic Science and Technology of China, Chengdu 610054 (China); Balfour, E.A. [School of Physical Electronics, University of Electronic Science and Technology of China, Chengdu 610054 (China); Hadimani, R.L.; Jiles, D.C. [Department of Electrical and Computer Engineering, Iowa State University, Ames, IA 50011 (United States); Ames Laboratory, US Department of Energy, Ames, IA 50011 (United States); Teng, B.H.; Luo, Y. [School of Physical Electronics, University of Electronic Science and Technology of China, Chengdu 610054 (China)

    2015-10-01

    This paper presents the structure, magnetic properties, and magnetocaloric effect of the polycrystalline compound GdNiAl{sub 2}. Powder X-ray diffraction (XRD) measurement and Rietveld refinement revealed that GdNiAl{sub 2} alloy is CuMgAl{sub 2}-type phase structure with about 1 wt% GdNi{sub 2}Al{sub 3} secondary phase. Magnetic measurements suggest that the compound is ferromagnetic and undergoes a second-order phase transition near 28 K. The maximum value of magnetic entropy change reaches 16.0 J/kg K for an applied magnetic field change of 0–50 kOe and the relative cooling power was 6.4×10{sup 2} J/kg. It is a promising candidate as a magnetocaloric material working near liquid hydrogen temperature (~20 K) exhibiting large relative cooling power. - Highlights: • Preferred orientation with axis of [010] was found in the GdNiAl{sub 2} compound. • The ΔS{sub Mmax} and the RCP are 16.0 J/kg K and 640 J/kg, respectively, for ΔH=50 kOe. • Relative low rare earth content in GdNiAl{sub 2} comparing with other candidates.

  15. Direct and indirect measurement of the magnetocaloric effect in a La0.6Ca0.4MnO3 ceramic perovskite

    DEFF Research Database (Denmark)

    Dinesen, A.R.; Linderoth, Søren; Mørup, Steen

    2002-01-01

    The adiabatic temperature change DeltaT(ad) due to a change of the external magnetic field (the magnetocaloric effect) for a perovskite-type La0.6Ca0.4MnO3 sample has been measured directly and indirectly (from the entropy change) and the results are compared. From the indirect method, involving ...

  16. Direct measurement of the magnetocaloric effect of microstructured Gd eutectic compounds using a new fast automatic device

    Science.gov (United States)

    Canepa, Fabio; Cirafici, Salvino; Napoletano, Myrta; Ciccarelli, Carlo; Belfortini, Claudio

    2005-01-01

    A newly designed experimental device for direct measurement of the magnetocaloric effect has been assembled and tested. Details about calibration and preliminary measurements performed on Gd as a standard reference material are reported together with results concerning the magnetocaloric effect of three different Gd eutectic compositions (Gd-Gd 7Pd 3, Gd-GdZn, Gd-GdCd).

  17. Large magnetocaloric effects in magnetic intermetallics: First-principles and Monte Carlo studies

    Directory of Open Access Journals (Sweden)

    Entel Peter

    2015-01-01

    Full Text Available We have performed ab initio electronic structure calculations and Monte Carlo simulations of frustrated ferroic materials where complex magnetic configurations and chemical disorder lead to rich phase diagrams. With lowering of temperature, we find a ferromagnetic phase which transforms to an antiferromagnetic phase at the magnetostructural (martensitic phase transition and to a cluster spin glass at still lower temperatures. The Heusler alloys Ni-(Co-Mn-(Cr-(Ga, Al, In, Sn, Sb are of particular interest because of their large inverse magnetocaloric effect associated with the magnetostructural transition and the influence of Co/Cr doping. Besides spin glass features, strain glass behavior has been observed in Ni-Co-Mn-In. The numerical simulations allow a complete characterization of the frustrated ferroic materials including the Fe-Rh-Pd alloys.

  18. Magnetization, ESR and large magnetocaloric effect in zigzag chain SrGd2O4

    Science.gov (United States)

    Jiang, X.; Ouyang, Z. W.; Wang, Z. X.; Xia, Z. C.; Rao, G. H.

    2018-01-01

    We performed the magnetization and electron spin resonance (ESR) measurements in the zigzag chain antiferromagnet SrGd2O4. First, the temperature-dependent ESR spectra suggest the presence of spin–spin correlations well above the ordering temperature due to geometric frustration. Second, the ESR data reveal the field-induced magnetic transition from an ordered state to a paramagnetic state, in accordance with the magnetization data. Third, the magnetization process exhibits a large magnetocaloric effect, which is associated with the alignment of paramagnetic spins along the direction of magnetic field. The maximum magnetic entropy change (‑ΔS M) near 3 K and refrigerant capacity (RCP) are 27 J · Kg‑1 · K‑1 and 325 J · Kg‑1, respectively, for a field change of 0–7 T. With negligible thermal and field hysteresis, SrGd2O4 can be considered as a cryogenic refrigerant material.

  19. Fluctuating local moments, itinerant electrons, and the magnetocaloric effect: Compositional hypersensitivity of FeRh

    Science.gov (United States)

    Staunton, J. B.; Banerjee, R.; Dias, M. dos Santos; Deak, A.; Szunyogh, L.

    2014-02-01

    We describe an ab initio disordered local moment theory for materials with quenched static compositional disorder traversing first-order magnetic phase transitions. It accounts quantitatively for metamagnetic changes and the magnetocaloric effect. For perfect stoichiometric B2-ordered FeRh, we calculate the transition temperature of the ferromagnetic-antiferromagnetic transition to be Tt= 495 K and a maximum isothermal entropy change in 2 T of |ΔS|=21.1 J K-1 kg-1. A large (40%) component of |ΔS| is electronic. The transition results from a fine balance of competing electronic effects which is disturbed by small compositional changes; e.g., swapping just 2% Fe of "defects" onto the Rh sublattice makes Tt drop by 290 K. This hypersensitivity explains the narrow compositional range of the transition and impurity doping effects.

  20. Investigation on the magnetocaloric effect in RNi{sub 2} (R: Dy, tb) melt-spun ribbon

    Energy Technology Data Exchange (ETDEWEB)

    Souza, M.V. de

    2016-08-15

    We report a theoretical and experimental investigation on the magnetocaloric properties of the rare earth RNi{sub 2} (R=Dy,Tb) in melt-spun ribbon and bulk form. The theoretical calculations were performed using a Hamiltonian model including the Zeeman-exchange interactions and the crystalline electrical field. Thus the magnetocaloric potential was calculated in the easy magnetic axes, in order an average over all of the possible directions. The isothermal entropy-change dependence on temperature calculated was compared with available experimental data for melt-spun ribbon and bulk material. We also investigated, theoretically and experimentally, the behavior of a DyNi{sub 2} and TbNi{sub 2} composite with optimized molar proportions and discussed this in the context of the optimum regeneration Ericsson cycle. - Highlights: • We investigate the effects of texture on the MCE of a melt-spun ribbon and a composite formed by RNi{sub 2} (R=Dy and Tb). • We compare the experimental data of MCE of a bulk and melt-spun ribbon. • We have successfully modeled the MCE in bulk and melt-spun ribbon considering the magnetic field applied along the easy magnetic axis and also averaged over all of the possible directions. • We describe a possible source of the increase in potential magnetocaloric.

  1. Strain-tuning of the magnetocaloric transition temperature in model FeRh films

    Science.gov (United States)

    Loving, M. G.; Barua, R.; Le Graët, C.; Kinane, C. J.; Heiman, D.; Langridge, S.; Marrows, C. H.; Lewis, L. H.

    2018-01-01

    The chemically ordered B2 phase of equiatomic FeRh is known to absorb or evolve a significant latent heat as it traverses its first-order phase transition in response to thermal, magnetic, and mechanical drivers. This attribute makes FeRh an ideal magnetocaloric material testbed for investigation of relationships between the crystalline lattice and the magnetic spins, which are especially experimentally accessible in thin films. In this work, epitaxial FeRh films of nominal 30 nm and 50 nm thicknesses with out-of-plane c-axis orientation were sputter-deposited at high temperature onto (0 0 1)-MgO or (0 0 0 1)-Al2O3 substrates and capped with Al, Au, Cr, or W after in situ annealing at 973 K to promote CsCl-type chemical order. In this manner a controlled strain state was invoked. Experimental results derived from laboratory and synchrotron x-ray diffraction combined with magnetometry indicate that the antiferromagnetic (AF)—ferromagnetic (FM) magnetostructural phase transformation in these films may be tuned over an ~50° range (373 K–425 K) through variation in the c/a ratio derived from lattice strain delivered by the substrate and the capping layers. These results supply fundamental information that might be used to engineer the magnetocaloric working material in new system designs by introducing targeted values of passive strain to the system.

  2. Giant magnetocaloric effect, magnetization plateaux and jumps of the regular Ising polyhedra

    International Nuclear Information System (INIS)

    Strečka, Jozef; Karľová, Katarína; Madaras, Tomáš

    2015-01-01

    Magnetization process and adiabatic demagnetization of the antiferromagnetic Ising spin clusters with the shape of regular polyhedra (Platonic solids) are exactly examined within the framework of a simple graph-theoretical approach. While the Ising cube as the only unfrustrated (bipartite) spin cluster shows just one trivial plateau at zero magnetization, the other regular Ising polyhedra (tetrahedron, octahedron, icosahedron and dodecahedron) additionally display either one or two intermediate plateaux at fractional values of the saturation magnetization. The nature of highly degenerate ground states emergent at intermediate plateaux owing to a geometric frustration is clarified. It is evidenced that the regular Ising polyhedra exhibit a giant magnetocaloric effect in a vicinity of magnetization jumps, whereas the Ising octahedron and dodecahedron belong to the most prominent geometrically frustrated spin clusters that enable an efficient low-temperature refrigeration by the process of adiabatic demagnetization

  3. Giant magnetocaloric effect, magnetization plateaux and jumps of the regular Ising polyhedra

    Energy Technology Data Exchange (ETDEWEB)

    Strečka, Jozef, E-mail: jozef.strecka@upjs.sk [Institute of Physics, Faculty of Science, P.J. Šafárik University, Park Angelinum 9, 040 01 Košice (Slovakia); Karľová, Katarína [Institute of Physics, Faculty of Science, P.J. Šafárik University, Park Angelinum 9, 040 01 Košice (Slovakia); Madaras, Tomáš [Institute of Mathematics, Faculty of Science, P.J. Šafárik University, Jesenná 5, 040 01 Košice (Slovakia)

    2015-06-15

    Magnetization process and adiabatic demagnetization of the antiferromagnetic Ising spin clusters with the shape of regular polyhedra (Platonic solids) are exactly examined within the framework of a simple graph-theoretical approach. While the Ising cube as the only unfrustrated (bipartite) spin cluster shows just one trivial plateau at zero magnetization, the other regular Ising polyhedra (tetrahedron, octahedron, icosahedron and dodecahedron) additionally display either one or two intermediate plateaux at fractional values of the saturation magnetization. The nature of highly degenerate ground states emergent at intermediate plateaux owing to a geometric frustration is clarified. It is evidenced that the regular Ising polyhedra exhibit a giant magnetocaloric effect in a vicinity of magnetization jumps, whereas the Ising octahedron and dodecahedron belong to the most prominent geometrically frustrated spin clusters that enable an efficient low-temperature refrigeration by the process of adiabatic demagnetization.

  4. Giant magnetocaloric effect, magnetization plateaux and jumps of the regular Ising polyhedra

    Science.gov (United States)

    Strečka, Jozef; Karľová, Katarína; Madaras, Tomáš

    2015-06-01

    Magnetization process and adiabatic demagnetization of the antiferromagnetic Ising spin clusters with the shape of regular polyhedra (Platonic solids) are exactly examined within the framework of a simple graph-theoretical approach. While the Ising cube as the only unfrustrated (bipartite) spin cluster shows just one trivial plateau at zero magnetization, the other regular Ising polyhedra (tetrahedron, octahedron, icosahedron and dodecahedron) additionally display either one or two intermediate plateaux at fractional values of the saturation magnetization. The nature of highly degenerate ground states emergent at intermediate plateaux owing to a geometric frustration is clarified. It is evidenced that the regular Ising polyhedra exhibit a giant magnetocaloric effect in a vicinity of magnetization jumps, whereas the Ising octahedron and dodecahedron belong to the most prominent geometrically frustrated spin clusters that enable an efficient low-temperature refrigeration by the process of adiabatic demagnetization.

  5. Conventional and inverse magnetocaloric effect in Pr2CuSi3 and Gd2CuSi3 compounds

    International Nuclear Information System (INIS)

    Wang, Fang; Yuan, Feng-ying; Wang, Jin-zhi; Feng, Tang-fu; Hu, Guo-qi

    2014-01-01

    Highlights: • Two phase transitions in a narrow temperature range were observed and studied. • Both typical and inverse magnetocaloric effect were observed and discussed. • The inverse magnetocaloric effect was attributed to the spin-glass behavior. - Abstract: Magnetic properties and magnetocaloric effect (MCE) in Pr 2 CuSi 3 and Gd 2 CuSi 3 compounds were investigated systematically. Both Pr 2 CuSi 3 and Gd 2 CuSi 3 compounds experienced two phase transitions in a relatively narrow temperature range: first a paramagnet (PM)–ferromagnet (FM) second-order phase transition at 12 and 26 K and then a FM–spin glass (SG) transition at 6 K and 7.5 K, respectively. The magnetic entropy change (ΔS M ) was calculated based on Maxwell relation using the collected magnetization data. The maximum of ΔS M for Pr 2 CuSi 3 and Gd 2 CuSi 3 compounds was 7.6 and 5 J kg −1 K −1 , respectively, at the applied filed change of 0–5 T. The shape of the temperature dependence of ΔS M (ΔS M –T) curve was obviously different from that of the conventional magnetic materials undergoing only one typical phase transition. In the left half part of ΔS M –T curve, ΔS M is not very sensitive to the applied field and they tend to intersect with the decrease of temperature. Both typical conventional and inverse MCE behavior were observed in Gd 2 CuSi 3 , which would be originated from the two transition features at the low temperatures

  6. Anisotropy of the magnetocaloric effect in DyNiAl

    Czech Academy of Sciences Publication Activity Database

    Kaštil, J.; Javorský, P.; Andreev, Alexander V.

    2009-01-01

    Roč. 321, č. 15 (2009), s. 2318-2321 ISSN 0304-8853 Institutional research plan: CEZ:AV0Z10100520 Keywords : magnetocaloric effec * DyNiAl * magnetism * anisotropy Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 1.204, year: 2009

  7. Magnetocaloric effect in high Gd content Gd-Fe-Al based amorphous/nanocrystalline systems with enhanced Curie temperature and refrigeration capacity

    Directory of Open Access Journals (Sweden)

    Linlin Zhang

    2016-03-01

    Full Text Available The Gd-Fe-Al amorphous/nanocrystalline composites were successfully designed and obtained with both high Curie temperature (Tc and large magnetic entropy change (ΔSM. The Tc can be tuned from 172 to 280 K and refrigeration capacity (RC has a value between 690 and 867 J/kg under a field change of 0–5 T by changing the Gd contents and the formation of Gd nanocrystallites. And, ΔSM in Gd-Fe-Al amorphous/nanocrystalline composites reached a value of 7.2 J kg−1 K−1 under a field change of 0–5 T. The high RC in Gd-Fe-Al system were ascribed to the widening full width at half maximum (δFWHM up to 240 K of the magnetic entropy change (ΔSMmax peak because of the combination contribution of amorphous matrix and the precipitated Gd-riched nanocrystalline. Our research would shed light on how to design attractive candidates for magnetic refrigeration materials with high performance at near room temperature.

  8. Magnetocaloric effect and magnetic properties in SmFe1-xMnxO3 perovskite: Monte Carlo simulations

    Science.gov (United States)

    Erchidi Elyacoubi, A. S.; Masrour, R.; Jabar, A.

    2018-03-01

    We have used Monte Carlo simulation to study the magnetocaloric effect on SmFe1-xMnxO3 perovskite. The temperature-dependent magnetization shows that the Néel temperature of the weak-ferromagnetic SmFeO3 decreases as Fe ions are substituted by Mn ions. A paramagnetic-to-weak-antiferromagnetic transition with decreasing the temperature is observed and the corresponding Néel temperature essentially decreases as the Mn content increases. The magnetocaloric effect shows two peaks related to magnetic behavior changes, at paramagnetic-like behavior TK(K) and at Néel temperature TN(K) of SmFe1-xMnxO3. The second phase transition is established. The magnetic entropy change is given for a several magnetic fields. We have also determined the relative cooling power for dilution x = 0.5 and for a several external magnetic fields. Finally, the magnetic hysteresis cycles have been obtained with different dilutions x and temperatures values.

  9. Magnetocaloric effect in La(FexSi1-x)13 doped with hydrogen and under external pressure

    International Nuclear Information System (INIS)

    Medeiros, L.G. de; Oliveira, N.A. de

    2006-01-01

    In this paper, we calculate the magnetocaloric effect in the compounds La(Fe x Si 1-x ) 13 doped with hydrogen and subjected to external pressure. We use a microscopical model where the Coulomb interaction between itinerant electrons is treated in the mean field approach. The effect of hydrogen atoms is considered as a chemical pressure. We also include phenomenologically the magnetoelastic coupling via the renormalization of the electron dispersion relation and the Debye temperature. The calculated isothermal entropy changes upon magnetic field variations for the compound La(Fe 0.88 Si 0.12 ) 13 H y are in good agreement with the available experimental data

  10. Magnetocaloric effect study of Pr0.67Ca0.33MnO3-La0.67Sr0.33MnO3 nanocomposite

    Science.gov (United States)

    Das, Kalipada; Roy Chowdhury, R.; Midda, S.; Sen, Pintu; Das, I.

    2018-03-01

    The present study involves investigaton of magnetocaloric effect of Pr0.67Ca0.33MnO3-La0.67Sr0.33MnO3 nanocomposite materials above room temperature. From application point of view in magnetic refrigeration our study highlights the enhancement of operating temperature region compared to the well known La0.67Sr0.33MnO3 refrigerant material above room temperature. Comparison has also been made with the magnetocaloric properties of La0.67Sr0.33MnO3 nanomaterials. The modification of the magnetocaloric entropy changes (broadening of the temperature dependent magnetic entropy change) is addressed due to the effect of the gradual melting of antiferromagnetic charge ordered state of the Pr0.67Ca0.33MnO3 nanoparticles in such nanocomposite materials.

  11. Magnetocaloric properties of distilled gadolinium: effects of structural inhomogeneity and hydrogen impurity

    Czech Academy of Sciences Publication Activity Database

    Burkhanov, G.S.; Kolchugina, N.B.; Tereshina, Evgeniya; Tereshina, I. S.; Politova, G.A.; Chzhan, V.B.; Badurski, D.; Chistyakov, O.D.; Paukov, M.; Drulis, H.; Havela, L.

    2014-01-01

    Roč. 104, č. 24 (2014), "242402-1"-"242402-5" ISSN 0003-6951 R&D Projects: GA ČR GAP204/12/0150 Institutional support: RVO:68378271 Keywords : high-purity rare-earth metals * gadolinium * magnetocaloric effect * hydrogenation * structural studies Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 3.302, year: 2014

  12. Indirect measurement of the magnetocaloric effect using a novel differential scanning calorimeter with magnetic field

    DEFF Research Database (Denmark)

    Jeppesen, Stinus; Linderoth, Søren; Pryds, Nini

    2008-01-01

    A simple and high-sensitivity differential scanning calorimeter (DSC) unit operating under magnetic field has been built for indirect determination of the magnetocaloric effect. The principle of the measuring unit in the calorimeter is based on Peltier elements as heat flow sensors. The high...

  13. Magnetocaloric effect in Mn2-pyrazole-[Nb(CN)8] molecular magnet by relaxation calorimetry

    Science.gov (United States)

    Pełka, R.; Gajewski, M.; Miyazaki, Y.; Yamashita, S.; Nakazawa, Y.; Fitta, M.; Pinkowicz, D.; Sieklucka, B.

    2016-12-01

    Magnetocaloric effect in {[Mn(pyrazole)4]2[Nb(CN)8]·4 H2O}n molecular magnet is reported. It crystallizes in tetragonal I41/a space group. The compound exhibits a phase transition to a long range magnetically ordered state at TN ≈ 22.8 K. Temperature dependences of the magnetic entropy change ΔSM as well as the adiabatic temperature change ΔTad due to applied field change μ0 ΔH in the range of 0.1-9 T have been inferred from the relaxation calorimetry measurements. A systematic approximate approach has been used to determine the lattice contribution to the heat capacity. The maximum value of ΔSM for μ0 ΔH = 5 T is 6.83 J mol-1 K-1 (6.65 J kg-1 K-1) at 24.3 K. The corresponding maximum value of ΔTad is 1.4 K at 23.8 K. The temperature dependence of the exponent n characterizing the field dependence of ΔSM has been estimated. It attains the value of 0.64 at the transition temperature, which is consistent with the 3D Heisenberg universality class. A hitherto unobserved two-peak structure has been revealed in the temperature dependence of ΔTad.

  14. Large roomtemperature magnetocaloric effect with negligible magnetic hysteresis losses in Mn1-xVxCoGe alloys

    International Nuclear Information System (INIS)

    Ma, S.C.; Zheng, Y.X.; Xuan, H.C.; Shen, L.J.; Cao, Q.Q.; Wang, D.H.; Zhong, Z.C.; Du, Y.W.

    2012-01-01

    The magnetic and magnetocaloric properties have been investigated in a series of Mn 1-x V x CoGe (x=0.01, 0.02, 0.03, and 0.05) alloys. The substitution of V for Mn reduces the structural transformation temperature of MnCoGe alloy effectively and results in a second-order magnetic transition in Mn 0.95 V 0.05 CoGe alloys. Large room temperature magnetocaloric effect and almost zero magnetic hysteresis losses are simultaneously achieved in the alloys with x=0.01, 0.02, and 0.03. The reasons for the negligible magnetic hysteresis losses and the potential application for the roomtemperature magnetic refrigeration are discussed. - Highlights: → V-substitution for Mn reduces the structural transformation temperature of MnCoGe. → FM-PM transition presents the second-order nature in Mn0.95V0.05CoGe. → The first-order FM-PM transitions are observed for alloys with x=0.01, 0.02, and 0.03. → Large room temperature MCEs are achieved in these alloys. → Negligible magnetic HL is achieved for these alloys simultaneously.

  15. Direct measurements of inverse magnetocaloric effects in metamagnetic shape-memory alloy NiCoMnIn

    Science.gov (United States)

    Kihara, T.; Xu, X.; Ito, W.; Kainuma, R.; Tokunaga, M.

    2014-12-01

    To clarify the electronic, lattice, and magnetic contribution to the inverse magnetocaloric effect (IMCE) in the metamagnetic shape-memory alloy Ni45Co5Mn50 -xInx, magnetization, magnetocaloric effect, and specific-heat measurements were carried out in a wide range of fields and temperatures. The IMCEs of Ni45Co5Mn36.7In13.3 were directly measured as adiabatic temperature changes in pulsed fields of up to 15 T. A maximum temperature decrease of -12.8 K was observed. The low-temperature specific heats in both the austenitic and the martensitic phases of Ni45Co5Mn36.5In13.5 were measured by using steady fields. Through analyses of the data, the entropy changes in charge (1.2 J/kg K), spin (-29 J/kg K), and lattice (51 J/kg K) sectors were individually evaluated. The result demonstrates the dominant role of the lattice sector in inverse MCEs in this material.

  16. The correlation of the magnetic properties and the magnetocaloric effect in (Gd1-xErx)NiAl alloys

    International Nuclear Information System (INIS)

    Korte, B.J.; Pecharsky, V.K.; Gschneidner, K.A. Jr.

    1998-01-01

    A study of the magnetic properties of several (Gd 1-x Er x )NiAl alloys (where x=0, 0.30, 0.40, 0.46, 0.50, 0.55, 0.60, 0.80, and 1.00) was undertaken using both ac and dc magnetic and heat capacity measurements in an attempt to understand the table-like magnetocaloric effect previously observed in (Gd 0.54 Er 0.46 )NiAl. Results indicate the presence of both antiferromagnetic and ferromagnetic ordering processes in all alloys containing Gd. For ErNiAl, a metamagnetic transition from an antiferromagnetic ground state was observed. Within each alloy, several magnetic transitions occur over a temperature range from 10 K [in (Gd 0.20 Er 0.80 )NiAl] up to 35 K (in GdNiAl), with all but the lowest temperature transition shifting to higher temperatures with increasing Gd content. The change in magnetic entropy (ΔS mag ) induced by a change in field is observed to peak around the Nacute eel temperature for ErNiAl while gradually broadening and shifting toward the Curie temperature as the Gd content is increased. For Gd-rich alloys, a significant contribution to ΔS mag is observed at both the low and high temperature transitions, resulting in a rounded, skewed caret-like temperature profile of the magnetocaloric effect. Factors, which are believed to contribute to this effect, include the presence and temperature spacing of multiple zero-field transitions, which most likely result from competing anisotropy and exchange interactions within a frustrated hexagonal spin lattice. This leads to broad peaks in the magnetic heat capacity that span several transition temperatures, providing for a substantial ΔS mag over an extended temperature range. This characteristic is desired for application to magnetic refrigeration, where certain thermodynamic cycles (e.g., Ericsson cycle) require specific temperature profiles of the magnetocaloric effect in refrigerant materials (e.g., a constant change in magnetic entropy as a function of temperature within the region of cooling). In

  17. High-throughput direct measurement of magnetocaloric effect based on lock-in thermography technique

    Science.gov (United States)

    Hirayama, Yusuke; Iguchi, Ryo; Miao, Xue-Fei; Hono, Kazuhiro; Uchida, Ken-ichi

    2017-10-01

    We demonstrate a high-throughput direct measurement method for the magnetocaloric effect (MCE) by means of a lock-in thermography (LIT) technique. This method enables systematic measurements of the magnetic-field and operation-frequency dependences of the temperature change induced by the MCE. This is accomplished in a shorter time compared to conventional adiabatic temperature measurement methods. The direct measurement based on LIT is free from any possible miscalculations and errors arising from indirect measurements using thermodynamic relations. Importantly, the LIT technique makes simultaneous MCE measurements of multiple materials possible without increasing the measurement time, realizing high-throughput investigations of the MCE. By applying this method to Gd, we obtain the MCE-induced temperature change of 1.84 ± 0.11 K under a modulation field of 1.0 T and modulation frequency of 0.5 Hz at a temperature of 300.5 ± 0.5 K, offering evidence that the LIT method gives quantitative results.

  18. Magnetocaloric effect of Er.sub.5./sub.Si.sub.4./sub. under hydrostatic pressure

    Czech Academy of Sciences Publication Activity Database

    Arnold, Zdeněk; Magen, C.; Morellon, L.; Algarabel, P.A.; Kamarád, Jiří; Ibarra, M. R.; Pecharsky, V. K.; Gschneidner, Jr., K. A.

    2009-01-01

    Roč. 79, č. 14 (2009), 144430/1-144430/6 ISSN 1098-0121 R&D Projects: GA ČR GA202/09/0030 Institutional research plan: CEZ:AV0Z10100521 Keywords : Curie temperature * entropy * erbium compounds * ferromagnetic materials * high-pressure solid-state phase transformations * magnetisation * magnetocaloric Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 3.475, year: 2009

  19. Direct measurement of the magnetocaloric effect in Tb5Si2Ge2

    International Nuclear Information System (INIS)

    Tocado, L.; Palacios, E.; Burriel, R.

    2005-01-01

    A method for measuring the adiabatic temperature change ΔT S upon quasi-static application of an external magnetic field H is proposed. ΔT S is directly measured with an accuracy better than 0.01K. Results of experiments on the giant magnetocaloric compound Tb 5 Si 2 Ge 2 are compared with those obtained from magnetization and heat capacity in an applied field

  20. The physical mechanism of magnetic field controlled magnetocaloric effect and magnetoresistance in bulk PrGa compound

    Science.gov (United States)

    Zheng, X. Q.; Wu, H.; Chen, J.; Zhang, B.; Li, Y. Q.; Hu, F. X.; Sun, J. R.; Huang, Q. Z.; Shen, B. G.

    2015-01-01

    The PrGa compound shows excellent performance on the magnetocaloric effect (MCE) and magnetoresistance (MR). The physical mechanism of MCE and MR in PrGa compound was investigated and elaborated in detail on the basis of magnetic measurement, heat capacity measurement and neutron powder diffraction (NPD) experiment. New types of magnetic structure and magnetic transition are found. The results of the NPD along with the saturation magnetic moment (MS) and magnetic entropy (SM) indicate that the magnetic moments are randomly distributed within the equivalent conical surface in the ferromagnetic (FM) temperature range. PrGa compound undergoes an FM to FM transition and an FM to paramagnetic (PM) transition as temperature increases. The magnetizing process was discussed in detail and the physical mechanism of the magnetic field controlled magnetocaloric effect (MCE) and the magnetoresistance (MR) was studied. The formation of the plateau on MCE curve was explained and MR was calculated in detail on the basis of the magnetic structure and the analysis of the magnetizing process. The experimental results are in excellent agreement with the calculations. Finally, the expression of MR = β(T)X2 and its application conditions were discussed, where X is M(H)/Meff, and Meff is the paramagnetic effective moment. PMID:26455711

  1. Critical behavior and reversible magnetocaloric effect in multiferroic MnCr2O4

    Science.gov (United States)

    Dey, K.; Indra, A.; Majumdar, S.; Giri, S.

    2017-08-01

    Magnetocaloric effect (MCE) in multiferroic cubic spinel MnCr2O4 (space group Fd 3 bar m, no. 227, cF56), has been investigated using dc magnetization studies. The values of maximum magnetic entropy change (Δ SMmax) and the adiabatic temperature change (Δ Tad) are ∼5.3 J kg-1 K-1 and ∼2 K, respectively, at ∼42.8 K for the magnetic field change of 50 kOe. The dc magnetization data near the transition temperature were analyzed by the modified Arrott plots, the Kouvel-Fisher method, log M vs log H, and the scaling analysis. Critical exponents β = 0.3932 ± 0.0287, γ = 1.0256 ± 0.0239, and δ = 3.55 ± 0.26 are obtained around the critical temperature ∼ 42.88 K. The critical exponents are in excellent agreement with the single scaling equation of state M (H, ɛ) =ɛ 0.3932 ± 0.0287 f± (H /ɛ ((0.3932 ± 0.0287) + (1.0256 ± 0.0239))); with f+ for T > 42.88 K, f- for T 3D Heisenberg model, while values of γ and δ are close to those of the mean field model. So the values of critical exponents indicate that the critical behavior of MnCr2O4 cannot be described within the framework of existing universality classes and probably belong to a separate class.

  2. Magnetocaloric effect and critical behaviour in Mn2-pyridazine-[Nb(CN)8] molecular compound under press.

    Science.gov (United States)

    Fitta, Magdalena; Bałanda, Maria; Pełka, Robert; Konieczny, Piotr; Pinkowicz, Dawid; Sieklucka, Barbara

    2013-12-11

    A comprehensive study of magnetocaloric effect (MCE) and critical behaviour in the ferrimagnetic Mn2–pyridazine–[Nb(CN)8] molecular magnet under hydrostatic pressure is reported. The pressure-induced structural changes provoke the strengthening of magnetic interaction between Mn and Nb centres. Consequently, an increase of critical temperature Tc is observed from 43 K for a sample at ambient pressure (A) to 52.5 K for a sample under a pressure of 1.19 GPa (AHP). The magnetocaloric effect was determined by the magnetization measurements. The application of a hydrostatic pressure of 1.19 GPa causes a decrease in the maximum value of magnetic entropy change ΔS, which for AHP is equal to 4.63 J mol−1 K−1 (7.73 J kg−1 K−1) at μ0ΔH = 5 T, while for A it is 5.36 J mol−1 K−1 (8.95 J kg−1 K−1) for the same magnetic field change. The temperature-dependent parameter n obtained for AHP, describing the field dependence of MCE, is consistent with other critical exponents determined from magnetization measurements. The critical exponents allow us to classify AHP to the 3D Heisenberg universality class, similar to the case of the non-pressurized sample.

  3. The normal and inverse magnetocaloric effect in RCu{sub 2} (R=Tb, Dy, Ho, Er) compounds

    Energy Technology Data Exchange (ETDEWEB)

    Zheng, X.Q., E-mail: zhengxq@ustb.edu.cn [School of Materials Science and Engineering, University of Science and Technology Beijing, Beijing 100083 (China); Xu, Z.Y. [National Institute of Metrology, Beijing 100029 (China); Zhang, B.; Hu, F.X. [State Key Laboratory for Magnetism, Institute of Physics, Chinese Academy of Sciences, Beijing 100190 (China); Shen, B.G., E-mail: shenbg@aphy.iphy.ac.cn [State Key Laboratory for Magnetism, Institute of Physics, Chinese Academy of Sciences, Beijing 100190 (China)

    2017-01-01

    Orthorhombic polycrystalline RCu{sub 2} (R=Tb, Dy, Ho and Er) compounds were synthesized and the magnetic properties and magnetocaloric effect (MCE) were investigated in detail. All of the RCu{sub 2} compounds are antiferromagnetic (AFM) ordered. As temperature increases, RCu{sub 2} compounds undergo an AFM to AFM transition at T{sub t} and an AFM to paramagnetic (PM) transition at T{sub N}. Besides of the normal MCE around T{sub N}, large inverse MCE around T{sub t} was found in TbCu{sub 2} compound. Under a field change of 0–7 T, the maximal value of inverse MCE is even larger than the value of normal MCE around T{sub N} for TbCu{sub 2} compound. Considering of the normal and inverse MCE, TbCu{sub 2} shows the largest refrigerant capacity among the RCu{sub 2} (R=Tb, Dy, Ho and Er) compounds indicating its potential applications in low temperature multistage refrigeration. - Highlights: • Large inverse magnetocaloric effect is observed in TbCu{sub 2} compound. • The AFM to AFM transition is observed in RCu{sub 2} (R=Tb, Dy, Ho, Er) compounds. • The MCE performance of TbCu{sub 2} compound is evaluated in a more comprehensively way.

  4. Tunable magneto-caloric effect in Gd1-xTbx heterostructures thin film

    Science.gov (United States)

    Lambert, C. H.; El Hadri, M. S.; Hamedoun, M.; Benyoussef, A.; Mounkachi, O.; Mangin, S.

    2017-12-01

    The magnetic and magneto-caloric properties of (Gd1-xTbx) alloy thin films and [Gd/Tb] multilayers have been investigated. All the samples had a total thickness of 100 nm and were deposited by DC sputtering. By changing the composition of the system, the ordering temperature (Tc) and the magnetic entropy changes of the compounds could be tuned. The results show that the Tc of the alloy thin films is close to 270 K for x = 0.2. Moreover, creating [Gd/Tb] multilayers with the same thickness and concentration of the studied Gd80Tb20 alloy film enables to strongly increase the relative cooling power, and reach values twice as big as from the corresponding alloys. These results suggest that nanostructuring of [Gd/Tb] multilayers may be a promising route to tailor the magnetocaloric response of materials.

  5. Magnetization process and magnetocaloric effect in geometrically frustrated Ising antiferromagnet and spin ice models on a 'Star of David' nanocluster

    Science.gov (United States)

    Žukovič, M.; Semjan, M.

    2018-04-01

    Magnetic and magnetocaloric properties of geometrically frustrated antiferromagnetic Ising (IA) and ferromagnetic spin ice (SI) models on a nanocluster with a 'Star of David' topology, including next-nearest-neighbor (NNN) interactions, are studied by an exact enumeration. In an external field applied in characteristic directions of the respective models, depending on the NNN interaction sign and magnitude, the ground state magnetization of the IA model is found to display up to three intermediate plateaus at fractional values of the saturation magnetization, while the SI model shows only one zero-magnetization plateau and only for the antiferromagnetic NNN coupling. A giant magnetocaloric effect is revealed in the IA model with the NNN interaction either absent or equal to the nearest-neighbor coupling. The latter is characterized by abrupt isothermal entropy changes at low temperatures and infinitely fast adiabatic temperature variations for specific entropy values in the processes when the magnetic field either vanishes or tends to the critical values related to the magnetization jumps.

  6. Effect of Zn doping on the magneto-caloric effect and critical constants of Mott insulator MnV2O4

    Science.gov (United States)

    Shahi, Prashant; Singh, Harishchandra; Kumar, A.; Shukla, K. K.; Ghosh, A. K.; Yadav, A. K.; Nigam, A. K.; Chatterjee, Sandip

    2014-09-01

    X-ray absorption near edge spectra (XANES) and magnetization of Zn doped MnV2O4 have been measured and from the magnetic measurement the critical exponents and magnetocaloric effect have been estimated. The XANES study indicates that Zn doping does not change the valence states in Mn and V. It has been shown that the obtained values of critical exponents β, γ and δ do not belong to universal class and the values are in between the 3D Heisenberg model and the mean field interaction model. The magnetization data follow the scaling equation and collapse into two branches indicating that the calculated critical exponents and critical temperature are unambiguous and intrinsic to the system. All the samples show large magneto-caloric effect. The second peak in magneto-caloric curve of Mn0.95Zn0.05V2O4 is due to the strong coupling between orbital and spin degrees of freedom. But 10% Zn doping reduces the residual spins on the V-V pairs resulting the decrease of coupling between orbital and spin degrees of freedom.

  7. Effect of Zn doping on the magneto-caloric effect and critical constants of Mott insulator MnV2O4

    Directory of Open Access Journals (Sweden)

    Prashant Shahi

    2014-09-01

    Full Text Available X-ray absorption near edge spectra (XANES and magnetization of Zn doped MnV2O4 have been measured and from the magnetic measurement the critical exponents and magnetocaloric effect have been estimated. The XANES study indicates that Zn doping does not change the valence states in Mn and V. It has been shown that the obtained values of critical exponents β, γ and δ do not belong to universal class and the values are in between the 3D Heisenberg model and the mean field interaction model. The magnetization data follow the scaling equation and collapse into two branches indicating that the calculated critical exponents and critical temperature are unambiguous and intrinsic to the system. All the samples show large magneto-caloric effect. The second peak in magneto-caloric curve of Mn0.95Zn0.05V2O4 is due to the strong coupling between orbital and spin degrees of freedom. But 10% Zn doping reduces the residual spins on the V-V pairs resulting the decrease of coupling between orbital and spin degrees of freedom.

  8. Low field magnetocaloric effect in bulk and ribbon alloy La(Fe0.88Si0.12)13

    Science.gov (United States)

    Vuong, Van-Hiep; Do-Thi, Kim-Anh; Nguyen, Duy-Thien; Nguyen, Quang-Hoa; Hoang, Nam-Nhat

    2018-03-01

    Low-field magnetocaloric effect occurred in itinerant metamagnetic materials is at core for magnetic cooling application. This works reports the magnetocaloric responses obtained at 1.35 T for the silicon-doped iron-based binary alloy La(Fe0.88Si0.12)13 in the bulk and ribbon form. Both samples possess a same symmetry but with different crystallite sizes and lattice parameters. The ribbon sample shows a larger maximum entropy change (nearly 8.5 times larger) and a higher Curie temperature (5 K higher) in comparison with that of the bulk sample. The obtained relative cooling power for the ribbon is also larger and very promising for application (RCP = 153 J/kg versus 25.2 J/kg for the bulk). The origin of the effect observed is assigned to the occurrence of negative magnetovolume effect in the ribbon structure with limit crystallization, caused by rapid cooling process at the preparation, which induced smaller crystallite size and large lattice constant at the overall weaker local crystal field.

  9. Magnetocaloric effect, thermal conductivity, and magnetostriction of epoxy-bonded La(Fe0.88Si0.12)13 hydrides

    Science.gov (United States)

    Matsumoto, K.; Murayama, D.; Takeshita, M.; Ura, Y.; Abe, S.; Numazawa, T.; Takata, H.; Matsumoto, Y.; Kuriiwa, T.

    2017-09-01

    Magnetic materials with large magnetocaloric effect are significantly important for magnetic refrigeration. La(Fe0.88Si0.12)13 compounds are one of the promising magnetocaloric materials that have a first order magnetic phase transition. Transition temperature of hydrogenated La(Fe0.88Si0.12)13 increased up to room temperature region while keeping metamagnetic transition properties. From view point of practical usage, bonded composite are very attractive and their properties are important. We made epoxy bonded La(Fe0.88Si0.12)13 hydrides. Magnetocaloric effect was studied by measuring specific heat, magnetization, and temperature change in adiabatic demagnetization. The composite had about 20% smaller entropy change from the hydrogenated La(Fe0.88Si0.12)13 powder in 2 T. Thermal conductivity of the composite was several times smaller than La(Fe,Si)13. The small thermal conductivity was explained due to the small thermal conductivity of epoxy. Thermal conductivity was observed to be insensitive to magnetic field in 2 T. Thermal expansion and magnetostriction of the composite material were measured. The composite expanded about 0.25% when it entered into ferromagnetic phase. Magnetostriction of the composite in ferromagnetic phase was about 0.2% in 5 T and much larger than that in paramagnetic phase. The composite didn’t break after about 100 times magnetic field changes in adiabatic demagnetization experiment even though it has magnetostriction.

  10. Europium substitution effects on structural, magnetic and magnetocaloric properties in La0.5Ca0.5MnO3

    Directory of Open Access Journals (Sweden)

    Boujelben W.

    2012-06-01

    Full Text Available We have investigated structural, magnetic and magnetocaloric properties of polycrystalline samples La0.5-xEuxCa0.5MnO3 (x=0 and 0.1. Rietveld refinement of the X-ray diffraction patterns show that our samples are single phase and crystallize in the orthorhombic structure with Pnma space group. Magnetization measurements versus temperature at a magnetic applied field of 500 Oe indicate that La0.4Eu0.1Ca0.5MnO3 sample exhibits a paramagnetic to ferromagnetic transition with decreasing temperature. Magnetic measurements reveal strong magnetocaloric effect in the vicinity of the Curie temperature TC. The parent compound shows a negative magnetic entropy change of ∆SM=−1.13Jkg−1K−1 at 220K and a positive magnetocaloric effects ∆SM=1Jkg−1K−1 at 150K under a magnetic applied field of 2T. La0.4Eu0.1Ca0.5MnO3 exhibits a maximum value of magnetic entropy change ∆SM=−1.15Jkg−1K−1 at 130K under an applied field of 2T and a large relative cooling power RCP with a maximum value of 72 J/kg.

  11. Magnetocaloric effect of Gd5 Si2 Ge2 alloys in low magnetic field

    Indian Academy of Sciences (India)

    Administrator

    (VSM) and a home-made magnetocaloric effect measuring apparatus, respectively. The maximum ΔSM of the alloys increases by 200% from 4⋅38 to 13⋅32 J kg–1 K–1, the maximum ΔTad increases by 105% from 1⋅9 to. 3⋅9 K when compared to the as-cast due to the homogeneous composition distribution and ...

  12. Practical system for the direct measurement of magneto-caloric effect by micro-thermocouples

    Czech Academy of Sciences Publication Activity Database

    Kamarád, Jiří; Kaštil, J.; Arnold, Zdeněk

    2012-01-01

    Roč. 83, č. 8 (2012), "083902-1"-"083902-7" ISSN 0034-6748 R&D Projects: GA ČR GAP204/12/0692 Institutional research plan: CEZ:AV0Z10100521 Keywords : copper * cryostats * magnetic transition * magnetic variables measurement * magnetocaloric effects * microsensors * permanent magnets * refrigeration Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 1.602, year: 2012

  13. Magnetocaloric effect of Gd-Tb alloys: influence of the sample shape anisotropy

    Czech Academy of Sciences Publication Activity Database

    Kaštil, J.; Javorský, J.; Kamarád, Jiří; Šantavá, Eva

    2011-01-01

    Roč. 104, č. 1 (2011), s. 205-209 ISSN 0947-8396 R&D Projects: GA ČR GA202/09/0030 Institutional research plan: CEZ:AV0Z10100521 Keywords : magnetic refrigeration * magnetization * specific heat * magnetocaloric effect * Gd-Tb alloy * shape anisotropy Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 1.630, year: 2011

  14. Determination of the entropy change using the acoustic detection technique in the investigation of the magnetocaloric effect

    Energy Technology Data Exchange (ETDEWEB)

    Soffner, M E; Mansanares, A M; Gandra, F C G; Coelho, A A [Instituto de Fisica Gleb Wataghin, Universidade Estadual de Campinas (UNICAMP), CP 6165, 13083-970, Campinas, SP (Brazil); Gama, S [Departamento de Ciencias Exatas e da Terra, Universidade Federal de Sao Paulo (UNIFESP), 09972-270, Diadema, SP (Brazil); Carvalho, A Magnus G; Pires, M J M [Instituto Nacional de Metrologia, Normalizacao e Qualidade Industrial (INMETRO), 25250-020, Duque de Caxias, RJ (Brazil); Guimaraes, A O; Silva, E C da, E-mail: manoel@ifi.unicamp.b [Laboratorio de Ciencias Fisicas, Universidade Estadual do Norte Fluminense Darcy Ribeiro, 28013-602, Campos dos Goytacazes, RJ (Brazil)

    2010-11-10

    In this paper we demonstrate the use of the acoustic detection as an alternative way to determine the entropy variation, {Delta}S{sub T}, a parameter normally used to characterize the magnetocaloric effect. The measurements were performed for a Gd sample in the 252-316 K temperature range for magnetic fields from zero up to 50 kOe. The reversible adiabatic curves were built in a T versus H diagram, and specific heat data obtained at zero-magnetic field were employed to assign the entropy values of each curve. Subsequently, the entropy was plotted as a function of temperature for fixed magnetic fields, and therefore the isothermal entropy variation, {Delta}S{sub T}, was found as a function of the temperature for several magnetic field steps.

  15. Thermodynamic behavior and enhanced magnetocaloric effect in a frustrated spin-1/2 Ising-Heisenberg triangular tube

    Science.gov (United States)

    Alécio, Raphael Cavalcante; Strečka, Jozef; Lyra, Marcelo L.

    2018-04-01

    The thermodynamic behavior of an Ising-Heisenberg triangular tube with Heisenberg intra-rung and Ising inter-rung interactions is exactly obtained in an external magnetic field within the framework of the transfer-matrix method. We report rigorous results for the temperature dependence of the magnetization, entropy, pair correlations and specific heat, as well as typical iso-entropic curves. The discontinuous field-driven ground-state phase transitions are reflected in some anomalous thermodynamic behavior as for instance a striking low-temperature peak of the specific heat and an enhanced magnetocaloric effect. It is demonstrated that the intermediate magnetization plateaus shrink in and the relevant sharp edges associated with the magnetization jump round off upon increasing temperature.

  16. Determination of the entropy change using the acoustic detection technique in the investigation of the magnetocaloric effect

    International Nuclear Information System (INIS)

    Soffner, M E; Mansanares, A M; Gandra, F C G; Coelho, A A; Gama, S; Carvalho, A Magnus G; Pires, M J M; Guimaraes, A O; Silva, E C da

    2010-01-01

    In this paper we demonstrate the use of the acoustic detection as an alternative way to determine the entropy variation, ΔS T , a parameter normally used to characterize the magnetocaloric effect. The measurements were performed for a Gd sample in the 252-316 K temperature range for magnetic fields from zero up to 50 kOe. The reversible adiabatic curves were built in a T versus H diagram, and specific heat data obtained at zero-magnetic field were employed to assign the entropy values of each curve. Subsequently, the entropy was plotted as a function of temperature for fixed magnetic fields, and therefore the isothermal entropy variation, ΔS T , was found as a function of the temperature for several magnetic field steps.

  17. The effects of substituting Ag for In on the magnetoresistance and magnetocaloric properties of Ni-Mn-In Heusler alloys

    Directory of Open Access Journals (Sweden)

    Sudip Pandey

    2016-05-01

    Full Text Available The effect of substituting Ag for In on the structural, magnetocaloric, and thermomagnetic properties of Ni50Mn35In15−xAgx (x = 0.1, 0.2, 0.5, and 1 Heusler alloys was studied. The magnitude of the magnetization change at the martensitic transition temperature (TM decreased with increasing Ag concentration. Smaller magnetic entropy changes (ΔSM were observed for the alloys with larger Ag concentrations and the martensitic transition shifted to higher temperature. A shift of TM by about 25 K to higher temperature was observed for an applied hydrostatic pressure of P = 6.6 kbar with respect to ambient pressure. A large drop in resistivity was observed for large Ag concentration. The magnetoresistance was dramatically suppressed due to an increase in the disorder of the system with increasing Ag concentration. Possible mechanisms responsible for the observed behavior are discussed.

  18. Direct measurements of conventional and anisotropic magnetocaloric effect in binary RAl2 single crystals

    Science.gov (United States)

    Monteiro, J. C. B.; Gandra, F. G.

    2017-06-01

    We report on specific heat and magnetocaloric effect (MCE) measurements in single crystals of HoAl2, DyAl2, and TbAl2 measured by a heat flux technique using Peltier devices. Those compounds order ferromagnetically at 31 K, 61 K, and 106 K respectively, and present a spin reorientation transition (SRT) below TC. We study the dependence of the SRT with magnetic field and temperature by means of specific heat measurements performed in single crystals oriented at the [" separators="| 100 ], [" separators="| 110 ], and [" separators="| 111 ] directions with the aid of calculations using a simple model. We obtained the conventional MCE for HoAl2 and TbAl2 and also the anisotropic version of the effect obtained indirectly from the specific heat for TbAl2 and DyAl2. We also present the results for a direct determination of the anisotropic MCE for DyAl2 by measuring the heat flux generated by a rotation of the single crystal under constant field.

  19. Negative thermal expansion and magnetocaloric effect in Mn-Co-Ge-In thin films

    Science.gov (United States)

    Liu, Y.; Qiao, K. M.; Zuo, S. L.; Zhang, H. R.; Kuang, H.; Wang, J.; Hu, F. X.; Sun, J. R.; Shen, B. G.

    2018-01-01

    MnCoGe-based alloys with magnetostructural transition show giant negative thermal expansion (NTE) behavior and magnetocaloric effects (MCEs) and thus have attracted a lot of attention. However, the drawback of bad mechanical behavior in these alloys obstructs their practical applications. Here, we report the growth of Mn-Co-Ge-In films with thickness of about 45 nm on (001)-LaAlO3, (001)-SrTiO3, and (001)-Al2O3 substrates. The films grown completely overcome the breakable nature of the alloy and promote its multifunctional applications. The deposited films have a textured structure and retain first-order magnetostructural transition. NTE and MCE behaviors associated with the magnetostructural transition have been studied. The films exhibit a completely repeatable NTE around room temperature. NTE coefficient α can be continuously tuned from the ultra-low expansion (α ˜ -2.0 × 10-7/K) to α ˜ -6.56 × 10-6/K, depending on the growth and particle size of the films on different substrates. Moreover, the films exhibit magnetic entropy changes comparable to the well-known metamagnetic films. All these demonstrate potential multifunctional applications of the present films.

  20. Magnetocaloric effect and critical behavior in Mn2-imidazole-[Nb(CN)8] molecular magnetic sponge

    Science.gov (United States)

    Fitta, Magdalena; Pełka, Robert; Gajewski, Marcin; Mihalik, Marian; Zentkova, Maria; Pinkowicz, Dawid; Sieklucka, Barbara; Bałanda, Maria

    2015-12-01

    A comprehensive study of magnetocaloric effect (MCE) and critical behavior in the {Mn2(imH)2(H2O)4[Nb(CN)8]·4H2O}n molecular magnet is reported. The compound is an example of a magnetic sponge, where structural changes provoked by dehydration process lead to the increase of Tc critical temperature from 25 K for the as-synthesized sample (1) up to 60 K for the anhydrous one (2). MCE and critical behavior were investigated by magnetization measurements. The maximum value of magnetic entropy change ΔS, determined by the magnetization measurements for 1 is 6.70 J mol-1 K-1 (8.95 J kg-1 K-1) at μ0ΔH=5 T, while for 2 it is equal to 4.02 J mol-1 K-1 (7.73 J kg-1 K-1) at the same magnetic field change. The field dependence of MCE at Tc for 1 and 2 was consistent with critical exponents, which allowed to classify both phases to 3D Heisenberg universality class. The Tc-2/3 dependence of the maximum entropy change has been tested using data of 1 and 2 together with MCE data previously reported for other members of the ferrimagnetic Mn2-L-[Nb(CN)8] (L=imidazole, pyridazine and pyrazole) series. Experimental MCE results have been compared with the spin contribution to the magnetic entropy change estimated using a molecular field approximation.

  1. Indirect measurement of the magnetocaloric effect using a novel differential scanning calorimeter with magnetic field.

    Science.gov (United States)

    Jeppesen, S; Linderoth, S; Pryds, N; Kuhn, L Theil; Jensen, J Buch

    2008-08-01

    A simple and high-sensitivity differential scanning calorimeter (DSC) unit operating under magnetic field has been built for indirect determination of the magnetocaloric effect. The principle of the measuring unit in the calorimeter is based on Peltier elements as heat flow sensors. The high sensitivity of the apparatus combined with a suitable calibration procedure allows very fast and accurate heat capacity measurements under magnetic field to be made. The device was validated from heat capacity measurements for the typical DSC reference material gallium (Ga) and a La(0.67)Ca(0.33)MnO(3) manganite system and the results were highly consistent with previous reported data for these materials. The DSC has a working range from 200 to 340 K and has been tested in magnetic fields reaching 1.8 T. The signal-to-noise ratio is in the range of 10(2)-10(3) for the described experiments. Finally the results have been compared to results from a Quantum Design(R) physical properties measuring system. The configuration of the system also has the advantage of being able to operate with other types of magnets, e.g., permanent magnets or superconducting coils, as well as the ability to be expanded to a wider temperature range.

  2. Magnetocaloric effect in M-pyrazole-[Nb(CN)(8)] (M = Ni, Mn) molecular compounds.

    Science.gov (United States)

    Fitta, Magdalena; Bałanda, Maria; Mihalik, Marian; Pełka, Robert; Pinkowicz, Dawid; Sieklucka, Barbara; Zentkova, Maria

    2012-12-19

    We report a study of magnetocaloric effect (MCE) in cyanido-bridged {[M(II)(pyrazole)(4)](2)[Nb(IV)(CN)(8)]·4H(2)O}(n) molecular compounds where M = Ni, Mn, pyrazole = C(3)H(4)N(2). The substances show a sharp phase transition to a long range magnetically ordered state, with ferromagnetic coupling between M and Nb sublattices in the case of the Ni-based sample 1 (T(c) = 13.4 K) and ferrimagnetic coupling for the Mn-based sample 2 (T(c) = 23.8 K). The magnetic entropy change ΔS due to applied field change ΔH as a function of temperature was determined by the magnetization and heat capacity measurements. The maximum value of ΔS at μ(0)ΔH = 5 T is 6.1 J mol(-1) K(-1) (5.9 J kg(-1) K(-1)) for 1 at T = 14 K and 6.7 J mol(-1) K(-1) (6.5 J kg(-1) K(-1)) for 2 at T = 25 K. MCE data at different applied fields have been presented as one universal curve, which confirms magnetic transitions in 1 and 2 to be of second order. The temperature dependences of the n exponent characterizing the dependence of ΔS on ΔH have been obtained. The n(T(c)) values, consistent with the shape of the magnetization curves, pointed to the 3D Heisenberg behaviour for 2 and some anisotropy, probably of the XY type, for 1. The (H/T(c))(2/3) dependence of the maximum entropy change has been tested in the ferrimagnetic Mn(2)-L-[Nb(CN)(8)] (L = C(3)H(4)N(2), C(4)H(4)N(2)) series.

  3. The magnetocaloric effect and critical behaviour of the Mn0.94Ti0.06CoGe alloy

    International Nuclear Information System (INIS)

    Shamba, P; Wang, J L; Debnath, J C; Zeng, R; Md Din, M F; Hong, F; Cheng, Z X; Dou, S X; Kennedy, S J; Studer, A J

    2013-01-01

    Structural, magnetic and magnetocaloric properties of the Mn 0.94 Ti 0.06 CoGe alloy have been investigated using x-ray diffraction, DC magnetization and neutron diffraction measurements. Two phase transitions have been detected, at T str = 235 K and T C = 270 K. A giant magnetocaloric effect has been obtained at around T str associated with a structural phase transition from the low temperature orthorhombic TiNiSi-type structure to the high temperature hexagonal Ni 2 In-type structure, which is confirmed by neutron study. In the vicinity of the structural transition, at T str , the magnetic entropy change, -ΔS M reached a maximum value of 14.8 J kg -1 K -1 under a magnetic field of 5 T, which is much higher than that previously reported for the parent compound MnCoGe. To investigate the nature of the magnetic phase transition around T C = 270 K from the ferromagnetic to the paramagnetic state, we performed a detailed critical exponent study. The critical components γ, β and δ determined using the Kouvel-Fisher method, the modified Arrott plot and the critical isotherm analysis agree well. The values deduced for the critical exponents are close to the theoretical prediction from the mean-field model, indicating that the magnetic interactions are long range. On the basis of these critical exponents, the magnetization, field and temperature data around T C collapse onto two curves obeying the single scaling equation M(H,ε) = ε β f ± (H/ε β+γ ).

  4. Effect of spin fluctuations in magnetocaloric and magnetoresistance properties of Dy10Co20Si70 alloy

    Science.gov (United States)

    Rashid, T. P.; Arun, K.; Curlik, Ivan; Ilkovic, Sergej; Reiffers, Marian; Dzubinska, Andrea; Nagalakshmi, R.

    2017-09-01

    Systematic investigations on the structure, magnetic, thermodynamic, magnetocaloric and magnetoresistance (MR) properties of the arc melted Dy10Co20Si70 alloy are presented. The Dy10Co20Si70 alloy crystallizes in tetragonal BaNiSn3-type DyCoSi3 (space group = I4mm; No. 107) as a major phase and CaF2-type CoSi2 (space group = Fm-3m; No. 225) and C-type Si (space group = Fd-3m; No. 227) as minor phases. The title compound exhibits multiple magnetic transitions having antiferromagnetic ordering at temperatures, viz., T1 = 10.8 K, T2 = 8.8 K and T3 = 3.3 K. The magnetic and thermodynamic studies confirm these magnetic anomalies in the compound. The large value of maximum magnetic entropy change, -ΔSMM a x = 16.4 and 26.6 J/kg K for the field change ΔH of 50 and 90 kOe, respectively, observed in the compound is associated with field induced magnetic transitions. Asymmetric broadening of the magnetic entropy change peaks above the ordering temperatures resulting in significant refrigerant capacities of 361 and 868 J/kg for ΔH = 50 and 90 kOe, respectively, in the compound is due to the spin fluctuation effect. The sign reversal in MR measurements is attributed to the field induced antiferromagnetic to ferromagnetic transition. A large positive MR (42% in 90 kOe) is observed at 2 K. The H2 dependence of both the magnetocaloric effect (MCE) and MR in the paramagnetic regime indicates the role of the applied magnetic field in suppressing the spin fluctuations. The large MCE and MR together with no thermal or magnetic hysteresis establish this new compound as an attractive multifunctional magnetic material.

  5. Magnetocaloric effect and multifunctional properties of Ni-Mn-based Heusler alloys

    Energy Technology Data Exchange (ETDEWEB)

    Dubenko, Igor, E-mail: igor_doubenko@yahoo.com [Department of Physics, Southern Illinois University, Carbondale, IL 62901 (United States); Samanta, Tapas; Kumar Pathak, Arjun [Department of Physics, Southern Illinois University, Carbondale, IL 62901 (United States); Kazakov, Alexandr; Prudnikov, Valerii [Faculty of Physics, Moscow State University, Vorob' evy Gory, 11999I Moscow (Russian Federation); Stadler, Shane [Department of Physics and Astronomy, Louisiana State University, Baton Rouge, LA 70803 (United States); Granovsky, Alexander [Faculty of Physics, Moscow State University, Vorob' evy Gory, 11999I Moscow (Russian Federation); IKERBASQUE, The Basque Foundation for Science, 48011 Bilbao (Spain); Departamento de Fisica de Materiales, Facultad de Quimica, Universidad del Pais Vasco, Paseo M. de Lardizabal 3, 20018 Donostia - San Sebastian (Spain); Zhukov, Arcady [IKERBASQUE, The Basque Foundation for Science, 48011 Bilbao (Spain); Departamento de Fisica de Materiales, Facultad de Quimica, Universidad del Pais Vasco, Paseo M. de Lardizabal 3, 20018 Donostia - San Sebastian (Spain); Ali, Naushad [Department of Physics, Southern Illinois University, Carbondale, IL 62901 (United States)

    2012-10-15

    The studies of magnetocaloric properties, phase transitions, and phenomena related to magnetic heterogeneity in the vicinity of the martensitic transition (MT) in Ni-Mn-In and Ni-Mn-Ga off-stoichiometric Heusler alloys are summarized. The crystal structure, magnetocaloric effect (MCE), and magnetotransport properties were studied for the following alloys: Ni{sub 50}Mn{sub 50-x}In{sub x}, Ni{sub 50-x}Co{sub x}Mn{sub 35}In{sub 15}, Ni{sub 50}Mn{sub 35-x}Co{sub x}In{sub 15}, Ni{sub 50}Mn{sub 35}In{sub 14}Z (Z=Al, Ge), Ni{sub 50}Mn{sub 35}In{sub 15-x}Si{sub x}, Ni{sub 50-x}Co{sub x}Mn{sub 25+y}Ga{sub 25-y}, and Ni{sub 50-x}Co{sub x}Mn{sub 32-y}FeyGa{sub 18}. It was found that the magnetic entropy change, {Delta}S, associated with the inverse MCE in the vicinity of the temperature of the magneto-structural transition, TM, persists in a range of (125-5) J/(kg K) for a magnetic field change {Delta}H=5 T. The corresponding temperature varies with composition from 143 to 400 K. The MT in Ni{sub 50}Mn{sub 50-x}In{sub x} (x=13.5) results in a transition between two paramagnetic states. Associated with the paramagnetic austenite-paramagnetic martensite transition {Delta}S=24 J/(kg K) was detected for {Delta}H=5 T at T=350 K. The variation in composition of Ni{sub 2}MnGa can drastically change the magnetic state of the martensitic phase below and in the vicinity of TM. The presence of the martensitic phase with magnetic moment much smaller than that in the austenitic phase above TM leads to the large inverse MCE in the Ni{sub 42}Co{sub 8}Mn{sub 32-y}FeyGa{sub 18} system. The adiabatic change of temperature ({Delta}T{sub ad}) in the vicinity of TC and TM of Ni{sub 50}Mn{sub 35}In{sub 15} and Ni{sub 50}Mn{sub 35}In{sub 14}Z (Z=Al, Ge) was found to be {Delta}T{sub ad}=-2 K and 2 K for {Delta}H=1.8 T, respectively. It was observed that |{Delta}T{sub ad}| Almost-Equal-To 1 K for {Delta}H=1 T for both types of transitions. The results on resistivity, magnetoresistance, Hall

  6. Magneto-caloric effect in the pseudo-binary intermetallic YPrFe{sub 17} compound

    Energy Technology Data Exchange (ETDEWEB)

    Alvarez, Pablo [Departamento de Fisica, Universidad de Oviedo, Calvo Sotelo, s/n, 33007 Oviedo (Spain); Gorria, Pedro, E-mail: pgorria@uniovi.es [Departamento de Fisica, Universidad de Oviedo, Calvo Sotelo, s/n, 33007 Oviedo (Spain); Sanchez Llamazares, Jose L. [Division de Materiales Avanzados, Instituto Potosino de Investigacion Cientifica y Tecnologica, Camino a la presa San Jose 2055, CP 78216, San Luis Potosi (Mexico); Perez, Maria J. [Departamento de Fisica, Universidad de Oviedo, Calvo Sotelo, s/n, 33007 Oviedo (Spain); Franco, Victorino [Departamento de Fisica de la Materia Condensada, ICMSE-CSIC, Universidad de Sevilla, P.O. Box 1065, 41080 Sevilla (Spain); Reiffers, Marian; Kovac, Jozef [Institute of Experimental Physics, Watsonova 47, SK-04001 Kosice (Slovakia); Puente-Orench, Ines [Institute Laue Langevin, 6 rue Jules Horowitz, 38042 Grenoble (France); Blanco, Jesus A. [Departamento de Fisica, Universidad de Oviedo, Calvo Sotelo, s/n, 33007 Oviedo (Spain)

    2011-12-15

    Highlights: Black-Right-Pointing-Pointer YPrFe{sub 17} exhibits a broad {Delta}S{sub M}(T) associated with the ferro-to-paramagnetic phase transition (T{sub C} Almost-Equal-To 290 K). Black-Right-Pointing-Pointer We obtain |{Delta}S{sub M}| Almost-Equal-To 2.3 J kg{sup -1} K{sup -1} and RCP Almost-Equal-To 100 J kg{sup -1}for a magnetic field change of 1.5 T. Black-Right-Pointing-Pointer A single master curve for {Delta}S{sub M} is found when compared with other isostructural R{sub 2}Fe{sub 17} binary alloys. - Abstract: We have synthesized the intermetallic YPrFe{sub 17} compound by arc-melting. X-ray and neutron powder diffraction show that the crystal structure is rhombohedral with R3{sup Macron }m space group (Th{sub 2}Zn{sub 17}-type). The investigated compound exhibits a broad isothermal magnetic entropy change {Delta}S{sub M}(T) associated with the ferro-to-paramagnetic phase transition (T{sub C} Almost-Equal-To 290 K). The |{Delta}S{sub M}| ( Almost-Equal-To 2.3 J kg{sup -1} K{sup -1}) and the relative cooling power ( Almost-Equal-To 100 J kg{sup -1}) have been calculated for applied magnetic field changes up to 1.5 T. A single master curve for {Delta}S{sub M} under different values of the magnetic field change can be obtained by a rescaling of the temperature axis. The results are compared and discussed in terms of the magneto-caloric effect in the isostructural R{sub 2}Fe{sub 17} (R = Y, Pr and Nd) binary intermetallic alloys.

  7. Magneto-caloric effect of a Gd50Co50 amorphous alloy near the freezing point of water

    Directory of Open Access Journals (Sweden)

    L. Xia

    2015-09-01

    Full Text Available In the present work, we report the magneto-caloric effect (MCE of a binary Gd50Co50 amorphous alloy near the freezing temperature of water. The Curie temperature of Gd50Co50 amorphous ribbons is about 267.5 K, which is very close to room temperature. The peak value of the magnetic entropy change (-ΔSmpeak and the resulting adiabatic temperature rise (ΔTad. of the Gd50Co50 amorphous ribbons is much higher than that of any other amorphous alloys previously reported with a Tc near room temperature. On the other hand, although the -ΔSmpeak of Gd50Co50 amorphous ribbons is not as high as those of crystalline alloys near room temperature, its refrigeration capacity (RC is still much larger than the RC values of these crystalline alloys. The binary Gd50Co50 amorphous alloy provides a basic alloy for developing high performance multi-component amorphous alloys near room temperature.

  8. Pressure effects on the magnetocaloric properties of MnFeP.sub.1-x./sub.As.sub.x./sub..

    Czech Academy of Sciences Publication Activity Database

    Brück, E.; Kamarád, Jiří; Sechovský, V.; Arnold, Zdeněk; Tegus, O.; De Boer, F. R.

    2007-01-01

    Roč. 310, - (2007), e1008-e1009 ISSN 0304-8853 Institutional research plan: CEZ:AV0Z10100521 Keywords : magnetic refrigeration * magnetocaloric effect * pressure effect * MnFe(P, As) compounds Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 1.704, year: 2007

  9. Effect of rapid quenching on the magnetism and magnetocaloric effect of equiatomic rare earth intermetallic compounds RNi (R = Gd, Tb and Ho)

    Energy Technology Data Exchange (ETDEWEB)

    Rajivgandhi, R. [Department of Physics, Indian Institute of Technology Madras, Chennai 600 036 (India); Arout Chelvane, J. [Defence Metallurgical Research Laboratory, Hyderabad 500 058 (India); Quezado, S.; Malik, S.K. [Departamento de F’ısica Teorica e Experimental, Universidade Federal do Rio Grande do Norte, Natal 59072-970 (Brazil); Nirmala, R., E-mail: nirmala@physics.iitm.ac.in [Department of Physics, Indian Institute of Technology Madras, Chennai 600 036 (India)

    2017-07-01

    Highlights: • Melt-spinning yields microcrystalline RNi (R = Gd, Tb and Ho) samples with texture. • The texture-induced anisotropy affects magnetic and magnetocaloric properties. • Melt-spinning helps one engineer magnetocaloric effect in rare-earth compounds. - Abstract: Magnetocaloric effect (MCE) in RNi (where R = Gd, Tb and Ho) compounds has been studied in their arc-melted and melt-spun forms. The compound GdNi has the orthorhombic CrB-type structure (Space group Cmcm, No. 63) and the compound HoNi has the orthorhombic FeB-type structure (Space group Pnma, No. 62) at room temperature regardless of their synthesis condition. However, arc-melted TbNi orders in a monoclinic structure (Space group P2{sub 1}/m, No. 11) and when it is rapidly quenched to a melt-spun form, it crystallizes in an orthorhombic structure (Space group Pnma, No. 62). The arc-melted GdNi, TbNi and HoNi compounds order ferromagnetically at ∼69 K, ∼67 K and ∼36 K (T{sub C}) respectively. While the melt-spun GdNi shows about 6 K increase in T{sub C}, the ordering temperature of TbNi remains nearly the same in both arc-melted and melt-spun forms. In contrast, a reduction in T{sub C} by about 8 K is observed in melt-spun HoNi, when compared to its arc-melted counterpart. Isothermal magnetic entropy change, ∆S{sub m}, calculated from the field dependent magnetization data indicates an enhanced relative cooling power (RCP) for melt-spun GdNi for field changes of 20 kOe and 50 kOe. A lowered RCP value is observed in melt-spun TbNi and HoNi. These changes could have resulted from the competing shape anisotropy and the granular microstructure induced by the melt-spinning process. Tailoring the MCE of rare earth intermetallic compounds by suitably controlled synthesis techniques is certainly one of the directions to go forward in the search of giant magnetocaloric materials.

  10. Multifunctional phenomena in rare-earth intermetallic compounds with a laves phase structure: giant magnetostriction and magnetocaloric effect

    Czech Academy of Sciences Publication Activity Database

    Tereshina, I.; Cwik, J.; Tereshina, Evgeniya; Politova, G.; Burkhanov, G.; Chzhan, V.; Ilyushin, A.; Miller, M.; Zaleski, A.; Nenkov, K.; Schultz, L.

    2014-01-01

    Roč. 50, č. 11 (2014), s. 2504604 ISSN 0018-9464 Institutional support: RVO:68378271 Keywords : giant magnetostriction * Laves phase structure * magnetic anisotropy * magnetocaloric effect * rare-earth intermetallic Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 1.386, year: 2014

  11. The anisotropic magnetocaloric effect described by Maxwell formulation: Application to DyAl{sub 2} and TbNi{sub 2}

    Energy Technology Data Exchange (ETDEWEB)

    Plaza, E.J.R., E-mail: ejrplaza@gmail.co [Instituto de Fisica ' Armando Dias Tavares' , Universidade do Estado do Rio de Janeiro - UERJ, Rua Sao Francisco Xavier, 524, 20550-013 RJ (Brazil); Sousa, V.S.R. de; Alho, B.P.; Ranke, P.J. von [Instituto de Fisica ' Armando Dias Tavares' , Universidade do Estado do Rio de Janeiro - UERJ, Rua Sao Francisco Xavier, 524, 20550-013 RJ (Brazil)

    2010-08-06

    In this work we present the Maxwell-like formulation of the anisotropic magnetocaloric effect for materials in single crystalline form subjected to a rotating applied magnetic field of constant intensity. This effect is a new topic in the magnetocaloric research area and can highlight some relevant mechanisms on spin reorientation. Application of the model to the ferromagnetic compounds DyAl{sub 2} and TbNi{sub 2}, which are subjected to cubic crystalline electric field anisotropy and isotropic exchange interaction, are performed. We obtain continuous and discontinuous reorientation transitions for the Cartesian components of magnetization which revealed some characteristics of the anisotropic magnetocaloric curves.

  12. Effect of vanadium doping on structural, magnetic and magnetocaloric properties of La{sub 0.5}Ca{sub 0.5}MnO{sub 3}

    Energy Technology Data Exchange (ETDEWEB)

    Mansouri, M., E-mail: mansourimoufida23@yahoo.fr [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, Sfax University, B.P. 1171, 3000 Sfax (Tunisia); Omrani, H. [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, Sfax University, B.P. 1171, 3000 Sfax (Tunisia); Cheikhrouhou-Koubaa, W. [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, Sfax University, B.P. 1171, 3000 Sfax (Tunisia); Centre de Recherche en Informatique, Multimédia et Traitement Numérique des Données, BP 275, Sakiet Ezzit, 3021 Sfax (Tunisia); Koubaa, M. [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, Sfax University, B.P. 1171, 3000 Sfax (Tunisia); Madouri, A. [Laboratoire de Photonique et Nanostructure, LPN-CNRS, Route de Nozay, 91460 Marcoussis (France); Cheikhrouhou, A. [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, Sfax University, B.P. 1171, 3000 Sfax (Tunisia)

    2016-03-01

    We report the effect of vanadium doping on structural, magnetic and magnetocaloric properties of La{sub 0.5}Ca{sub 0.5}Mn{sub 1−x}V{sub x}O{sub 3} (x=0.05; 0.1). Our samples were elaborated using the conventional solid state reaction method at high temperatures. X-Ray powder diffraction at room temperature indicates that our samples crystallize in the orthorhombic structure with Pbnm space group. Magnetic measurements reveal a paramagnetic-ferromagnetic transition with decreasing temperature. Magnetocaloric studies show that the maximum of the magnetic entropy change and the relative cooling power (RCP) are found to be 2.42 J Kg{sup −1} K{sup −1} and 162.75 J Kg{sup −1} for x=0.05 and 3.12 J Kg{sup −1} K{sup −1} and 221.31 J Kg{sup −1} for x=0.1 under a field change of 5 T. - Highlights: • The La{sub 0.5}Ca{sub 0.5}Mn{sub 1−x}V{sub x}O{sub 3}(x=0.05 and x=0.1) compounds were synthesized using conventional solid state reaction method. • T{sub C} increases with V content from 187 K for x=0.05 to 263 K for x=0.1 • Large magnetocaloric effect is reported based on second order phase transition. • Noticeable |∆S{sub M}| at 5 T field makes the system useful for magnetic refrigeration.

  13. Magnetocaloric effect in perovskite manganite Nd0.6La0.1Sr0.3MnO3

    International Nuclear Information System (INIS)

    Fan Jiyu; Ling, Langsheng; Hong Bo; Pi Li; Zhang Yuheng

    2009-01-01

    In this paper, the magnetocaloric effect of perovskite manganite Nd 0.6 La 0.1 Sr 0.3 MnO 3 has been investigated. From the measurement of isothermal magnetization around the Curie temperature, we have calculated the maximum isothermal magnetic entropy change as 3.14 J/kg K for the 1.5 T magnetic field variation. Furthermore, a large relative cooling power of 45 J/kg has been determined, which makes Nd 0.6 La 0.1 Sr 0.3 MnO 3 attractive candidate materials for magnetic refrigeration.

  14. Experimental investigation of small-scale magnetocaloric refrigerator

    Czech Academy of Sciences Publication Activity Database

    Kaštil, Jiří; Tětek, J.; Tuček, A.

    2013-01-01

    Roč. 124, č. 4 (2013), s. 740-744 ISSN 0587-4246 Institutional support: RVO:68378271 Keywords : magnetocaloric refrigerator * magnetocaloric effect Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 0.604, year: 2013

  15. A comparative study of critical phenomena and magnetocaloric properties of ferromagnetic ternary alloys

    Science.gov (United States)

    Yüksel, Yusuf; Akinci, Ümit

    2018-01-01

    Magnetic and magnetocaloric properties, as well as the phase diagrams of a ferromagnetic ternary alloy system have been studied. A detailed comparison of two different methods, namely the effective field theory (EFT), and Monte Carlo (MC) simulations has been provided. Our numerical data show that the general qualitative picture presented by two methods are in a good agreement with each other. In terms of the magnetocaloric properties, our results yield that it is possible to design magnetic materials with a variety of working temperatures and magnetocaloric properties (such as large ΔSM and q values) by manipulating the magnetic phase transition via tuning the compositional factor (i.e. the mixing ratio of sublattice ions). The observed magnetocaloric effect has been found to be a direct one with ΔSM < 0 associated with a second order phase transition.

  16. Table-like magnetocaloric effect of Fe88−xNdxCr8B4 composite materials

    International Nuclear Information System (INIS)

    Lai, J.W.; Zheng, Z.G.; Zhong, X.C.; Franco, V.; Montemayor, R.; Liu, Z.W.; Zeng, D.C.

    2015-01-01

    The narrow working temperature range due to the sharp magnetic entropy change |ΔS M | peak and large thermal or magnetic hysteresis restricts the practical application of magnetocaloric materials. In this work, the table-like magnetocaloric effect (MCE) was obtained in the multilayer composite of Fe 88−x Nd x Cr 8 B 4 alloys with various Nd substitutions for Fe (x=5, 8, 10, 12, and 15), which were prepared by arc-melting followed by melt-spinning. The substation of Nd was found to enhance the glass-forming ability. For the alloys with Nd substitution from 5 at% to 15 at%, the Curie temperature (T C ) ranged from 322 K to 350 K and the peak value of |ΔS M | remained almost constant, 3.4–3.5 J/(kg K) under an applied field of 0–5 T. The composite with various Nd contents was prepared by stocking the ribbons layer by layer. The |ΔS M | of the composite approached a nearly constant value of ∼3.2 J/(kg K) in a field change of 0–5 T in a wide temperature span over 40 K, resulting in large refrigerant capacity value of >408 J/kg. This |ΔS M | value was much larger than the previous reported Fe-based amorphous composite Fe 78−x Ce x Si 4 Nb 5 B 12 Cu 1 . This composite can be used as the working material in the Ericsson-cycle magnetic regenerative refrigerator around room temperature. - Highlights: • The T C ranges from 322 K to 350 K when increasing Nd substitution from 5 to 15 at%. • |ΔS M | remains relatively constant, about 3.4–3.5 J/(kg K) under H=0–5 T. • RC decreases from 93 to 78 J/kg in a field change of 1.5 T when Nd increasing. • Table-like MCE ,|ΔS M | ~3.2J/kg K under 0–5 T, appeared in the composite. • A wide working temperature range (40 K) and enhanced RC (>408J/kg) were obtained in the composite

  17. Magnetocaloric effects of binary rare earth mononitrides, Gd {sub x}Tb{sub 1-x}N and Tb {sub x}Ho{sub 1-x}N

    Energy Technology Data Exchange (ETDEWEB)

    Nakagawa, Takashi [Department of Nuclear Engineering, Graduate School of Engineering, Osaka University, Yamadaoka 2-1, Suita, Osaka 565-0871 (Japan)]. E-mail: nakagawa@mit.eng.osaka-u.ac.jp; Sako, Kengo [Department of Nuclear Engineering, Graduate School of Engineering, Osaka University, Yamadaoka 2-1, Suita, Osaka 565-0871 (Japan); Arakawa, Takayuki [Department of Nuclear Engineering, Graduate School of Engineering, Osaka University, Yamadaoka 2-1, Suita, Osaka 565-0871 (Japan); Tomioka, Naoto [Department of Nuclear Engineering, Graduate School of Engineering, Osaka University, Yamadaoka 2-1, Suita, Osaka 565-0871 (Japan); Yamamoto, Takao A. [Department of Nuclear Engineering, Graduate School of Engineering, Osaka University, Yamadaoka 2-1, Suita, Osaka 565-0871 (Japan); Kamiya, Koji [Tsukuba Magnet Laboratory, National Institute for Materials Science, Tsukuba, Ibaraki 305-0003 (Japan); Numazawa, Takenori [Tsukuba Magnet Laboratory, National Institute for Materials Science, Tsukuba, Ibaraki 305-0003 (Japan)

    2006-02-09

    We have synthesized Gd {sub x}Tb{sub 1-x}N and Tb {sub x}Ho{sub 1-x}N (x = 0, 0.25, 0.5, 0.75 and 1) by the carbothermic reduction performed in a nitrogen gas stream. GdN and TbN have been completely miscible with each other as well as TbN and HoN. As x was changed from 0 to 1, the Curie temperature increased monotonously from 18.5 to 43.8 K for Tb {sub x}Ho{sub 1-x}N and from 43.8 to 61.2 K for Gd {sub x}Tb{sub 1-x}N. The magnetocaloric effects have been evaluated by calculating the magnetic entropy changes from the magnetization data sets measured at different applied fields and temperatures. In any composition x, the magnetocaloric effects of Gd {sub x}Tb{sub 1-x}N and Tb {sub x}Ho{sub 1-x}N are larger than those of Gd {sub x}Dy{sub 1-x}N. Therefore, Gd {sub x}Tb{sub 1-x}N and Tb {sub x}Ho{sub 1-x}N are promising magnetic refrigerant materials for hydrogen liquefying system working below liquid nitrogen temperature.

  18. Magnetocaloric effect in rare-earth intermetallics: Recent trends

    Indian Academy of Sciences (India)

    2015-05-27

    and adiabatic temperature (ad) that accompany magnetic transitions in materials during the application or the removal of magnetic field under adiabatic conditions. The physics of MCE gets enriched by correlated ...

  19. Improvement of magnetocaloric properties of Gd-Ge-Si alloys by alloying with iron

    Directory of Open Access Journals (Sweden)

    Erenc-Sędziak T.

    2013-01-01

    Full Text Available The influence of annealing of Gd5Ge2Si2Fex alloys at 1200°C and of alloying with various amount of iron on structure as well as thermal and magnetocaloric properties is investigated. It was found that annealing for 1 to 10 hours improves the entropy change, but reduces the temperature of maximum magnetocaloric effect by up to 50 K. Prolonged annealing of the Gd5Ge2Si2 alloy results in the decrease of entropy change due to the reduction of Gd5Ge2Si2 phase content. Addition of iron to the ternary alloy enhances the magnetocaloric effect, if x = 0.4 – 0.6, especially if alloying is combined with annealing at 1200°C: the peak value of the isothermal entropy change from 0 to 2 T increases from 3.5 to 11 J/kgK. Simultaneously, the temperature of maximum magnetocaloric effect drops to 250 K. The changes in magnetocaloric properties are related to the change in phase transformation from the second order for arc molten ternary alloy to first order in the case of annealed and/or alloyed with iron. The results of this study indicate that the minor addition of iron and heat treatment to Gd-Ge-Si alloys may be useful in improving the materials’ magnetocaloric properties..

  20. The effect of demagnetization on the magnetocaloric properties of gadolinium

    DEFF Research Database (Denmark)

    Bahl, Christian Robert Haffenden; Nielsen, Kaspar Kirstein

    2009-01-01

    of gadolinium. The adiabatic temperature change DeltaTad of gadolinium sheets upon application of a magnetic field has been measured at a range of applied magnetic fields and sample orientations. A significant dependence of DeltaTad on the sample orientation is observed. This can be accounted...... for by the demagnetization factor. Also, the temperature dependence of DeltaTad has been measured experimentally and modeled by mean field theory. Corrections to mean field theory modeling due to the demagnetization field are proposed and discussed. ©2009 American Institute of Physics...

  1. Theoretical approach to the magnetocaloric effect with hysteresis

    International Nuclear Information System (INIS)

    Basso, V.; Bertotti, G.; LoBue, M.; Sasso, C.P.

    2005-01-01

    In this paper a thermodynamic model with internal variables is presented and applied to ferromagnetic hysteresis. The out-of-equilibrium Gibbs free energy of a magnetic system is expressed as a function of the internal state of the Preisach model. Expressions for the system entropy and the entropy production are derived. By this approach it is possible to reproduce the characteristic features of the experimentally observed temperature changes (of the order of 10 -4 K around room temperature) induced by the magnetic field along the hysteresis loop performed in iron under adiabatic condition

  2. Critical behavior and magnetocaloric effect of Pr1-xCaxMnO3

    Science.gov (United States)

    Ho, T. A.; Thanh, T. D.; Yu, Yikyung; Tartakovsky, D. M.; Ho, T. O.; Thang, P. D.; Le, Anh-Tuan; Phan, The-Long; Yu, S. C.

    2015-05-01

    The critical behavior of Pr1-xCaxMnO3 samples with x = 0.25, 0.27, and 0.29 has been investigated. Detailed analyses of magnetic-field dependences of magnetization at temperatures around the paramagnetic-ferromagnetic transition, M(H, T), reveal that the samples undergo a second-order magnetic phase transition. The Arrott plot method predicts the values of critical parameters to be TC ≈ 118 K, β = 0.351 ± 0.003, γ = 1.372 ± 0.002, and δ = 4.90 ± 0.02 for x = 0.25; TC ≈ 116 K, β = 0.362 ± 0.002, γ = 1.132 ± 0.004, and δ = 4.09 ± 0.03 for x = 0.27; and TC ≈ 110 K, β = 0.521 ± 0.002, γ = 0.912 ± 0.005, and δ = 2.71 ± 0.02 for x = 0.29. The values of β = 0.351 (for x = 0.25) and β = 0.362 (for x = 0.27) are close to the value β = 0.365 expected for the 3D Heisenberg model, proving an existence of short-range ferromagnetic interactions in these samples. A slight increase in Ca-doping content (x = 0.29) leads to the shift of the β value (=0.521) towards that of the mean-field theory (with β = 0.5) characteristic of long-range ferromagnetic interactions. The samples also exhibit a magnetocaloric effect: around TC of Pr1-xCaxMnO3 compounds, magnetic-entropy change reaches the maximum values of about 5.0, 4.1, and 2.5 J kg-1 K-1 for x = 0.25, 0.27, and 0.29, respectively, under an applied-field change of 50 kOe. Magnetic-field dependences of the maximum magnetic-entropy change (ΔSmax) obey a power law |ΔSmax(H)| ∝ Hn, where exponent values n = 0.68-0.74 are close to those obtained from the theoretical relation n = 1 + (β - 1)/(β + γ).

  3. Giant magnetocaloric effect in Gd5(Si2Ge2 alloy with low purity Gd

    Directory of Open Access Journals (Sweden)

    Cleber Santiago Alves

    2004-12-01

    Full Text Available Gd5(Ge1-xSi x, x < 4 based alloys are potential candidates for magnetic refrigeration in the range ~20 - ~290 K. However, one of the greatest obstacles for the use of that technology in large scale is the utilization of high pure Gd metal (99.99 wt. (% to produce the GdGeSi alloys, since the impurity elements decrease the intensity of the magnetocaloric effect (EMC¹. In this work, we prove that annealing of the Gd5Ge2Si2 can promote remarkable values for the EMC in comparison to those obtained for the alloy with high pure Gd. Also, the as cast alloy and the annealed alloy are not monophasic, but have at least two crystalline phases in their microstructure. Results for X-ray analysis, optical and electronic microscopy and magnetization measurements are reported.

  4. Magnetocaloric effect in ferromagnetic and ferrimagnetic systems under first and second order phase transition

    Energy Technology Data Exchange (ETDEWEB)

    Ranke, P.J. von, E-mail: von.ranke@uol.com.b [Instituto de Fisica ' Armando Dias Tavares' , Universidade do Estado do Rio de Janeiro-UERJ, Rua Sao Francisco Xavier, 524, 20550-013 RJ (Brazil); Oliveira, N.A. de; Alho, B.P.; Sousa, V.S.R. de; Plaza, E.J.R. [Instituto de Fisica ' Armando Dias Tavares' , Universidade do Estado do Rio de Janeiro-UERJ, Rua Sao Francisco Xavier, 524, 20550-013 RJ (Brazil); Carvalho, A. Magnus G. [Divisao de Metrologia de Materiais, Instituto Nacional de Metrologia, Normalizacao e Qualidade Industrial, Duque de Caxias, RJ (Brazil)

    2010-01-15

    In this work we present a model to describe the magnetocaloric effect (MCE) in ferrimagnetic arrangements. Our model takes into account the magnetoelastic interactions in the two coupled magnetic sublattices, which can lead to the onset of the first order magnetic phase transition and the giant-MCE. Several profiles of the MCE, such as: the inverse- and giant-MCE were systematically studied. Application of the model to the ferromagnetic compounds GdAl{sub 2}, Gd{sub 5}(Ge{sub 1.72}Si{sub 2.28}), Gd{sub 5}(Ge{sub 2}Si{sub 2}), and to the ferrimagnetic compound Y{sub 3}Fe{sub 5}O{sub 12} was performed, showing a good agreement with the experimental data.

  5. Critical magnetic behavior and large magnetocaloric effect in Pr0.67Ba0.33MnO3 perovskite manganite

    Science.gov (United States)

    Varvescu, A.; Deac, I. G.

    2015-08-01

    We report results of critical magnetic behavior and magnetocaloric investigations of the perovskite manganite Pr0.67Ba0.33MnO3. The compound exhibits a paramagnetic (PM) to ferromagnetic (FM) transition at the Curie temperature TC, and significant negative magnetoresistance in a wide temperature range. To probe the magnetic interactions responsible for the magnetic transitions, we performed a critical exponent analysis in the vicinity of the FM-PM transition region. Magnetic entropy change ΔSM was estimated from isothermal magnetization data. We have found a remarkable large value of |ΔSM| around TC's, of about 5.50 J/kg K for μ0ΔH=4 T and a large relative cooling power (~225 J/kg). The analysis was done by using the modified Arrot plot (MAP) method. The values of the obtained critical exponents associated with this transition, β=0.366, γ=1.375 and δ=4.743 are close to those expected for the short range 3D Heisenberg model. The model was also confirmed by using |ΔSM|∝(μ0H)n, the field dependence of magnetic entropy change method. The large measured magnetocaloric effect is presumed to arise as a consequence of the sample preparation route.

  6. Engineered Gd-Co based multilayer stack to enhanced magneto-caloric effect and relative cooling power

    Science.gov (United States)

    Tadout, M.; Lambert, C.-H.; El Hadri, M. S.; Mounkachi, O.; Benyoussef, A.; Hamedoun, M.; Benaissa, M.; Mangin, S.

    2018-02-01

    Magnetic refrigeration based on the magneto-caloric effect is one of the best alternatives to compete with vapor-compression technology. The viability of a magnetic refrigeration system for magnetic cooling can be tested by exploiting the materials in various forms, ranging from bulk to nanostructured materials. In order to achieve a wide refrigerating temperature range in magnetic refrigeration, we study in this paper a 100 nm-thick Gd-Co alloys-based multilayer stack. The stack is made of four individual Gd-Co alloy layers with different values of concentration and Curie temperature (TC). A magnetic entropy change associated with the second-order magnetic phase transition was determined from the magnetic isotherms. Moreover, the relative cooling power (RCP) of the studied Gd-Co-based multilayer is enhanced compared to the one of bulk Gd, and reaches a value of 200 J/kg. Such an enhancement of the RCP is not due to an enhanced maximum variation of entropy, but this is due to a much broader magnetic entropy peak. This study demonstrates the potential of nanostructured Gd-Co multilayer stack for magnetic cooling applications.

  7. On the electronic origin of the inverse magnetocaloric effect in Ni-Co-Mn-In Heusler alloys

    Czech Academy of Sciences Publication Activity Database

    Vasiliev, A. N.; Heczko, Oleg; Volkova, O.S.; Vasilchikova, T.N.; Voloshok, T.N.; Klimov, K.V.; Ito, W.; Kainuma, R.; Ishida, K.; Oikawa, K.; Fähler, S.

    2010-01-01

    Roč. 43, č. 5 (2010), 055004/1-055004/7 ISSN 0022-3727 Grant - others:AV ČR(CZ) M100100913 Institutional research plan: CEZ:AV0Z10100520 Keywords : inverse magnetocaloric effect * magnetically induced martensitic transformation * magnetic and transport properties * Ni-Mn-In-Co Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 2.105, year: 2010 http://iopscience.iop.org/0022-3727/43/5/055004/

  8. Low field induced large magnetocaloric effect in Tm2Ni0.93Si2.93 : influence of short range magnetic correlation.

    Science.gov (United States)

    Pakhira, Santanu; Mazumdar, Chandan; Ranganathan, R

    2017-10-31

    In this work, we report successful synthesis of a new intermetallic compound Tm2Ni0.93Si2.93 that forms in single phase only in defect crystal structure. The compound does not show any long range magnetic ordering down to 2 K. The material exhibits large magnetic entropy change (-ΔSM ~ 13.7 J/kg K) and adiabatic temperature change (ΔTad ~ 4.4 K) at 2.2 K for a field change of 20 kOe which can be realized by permanent magnets, thus being very beneficial for application purpose. In the absence of long range magnetic ordering down to 2 K, metastable nature of the low temperature spin dynamics and short range magnetic correlations are considered to be responsible for such large magnetocaloric effect (MCE) over a wide temperature region. © 2017 IOP Publishing Ltd.

  9. Low-field induced large magnetocaloric effect in Tm2Ni0.93Si2.93: influence of short-range magnetic correlation.

    Science.gov (United States)

    Pakhira, Santanu; Mazumdar, Chandan; Ranganathan, R

    2017-11-20

    In this work, we report the successful synthesis of a new intermetallic compound Tm 2 [Formula: see text] [Formula: see text] that forms in single phase only in defect crystal structure. The compound does not show any long range magnetic ordering down to 2 K. The material exhibits a large magnetic entropy change ([Formula: see text] J [Formula: see text] K -1 ) and adiabatic temperature change ([Formula: see text] K) at 2.2 K for a field change of 20 kOe which can be realized by permanent magnets, thus being very beneficial for application purpose. In the absence of long-range magnetic ordering down to 2 K, the metastable nature of low-temperature spin dynamics and short-range magnetic correlations are considered to be responsible for such a large magnetocaloric effect over a wide temperature region.

  10. Tunable magnetic properties and magnetocaloric effect of off-stoichiometric LaMnO3 nanoparticles

    Science.gov (United States)

    Tola, P. S.; Kim, H. S.; Kim, D. H.; Phan, T. L.; Rhyee, J. S.; Shon, W. H.; Yang, D. S.; Manh, D. H.; Lee, B. W.

    2017-12-01

    The crystal and electronic structures and the magnetic and magnetocaloric properties of off-stoichiometric LaMnO3 nanoparticles (NPs) with various particle sizes D = 20-100 nm were studied. The Rietveld refinement revealed that all NPs were crystallized in the rhombohedral structure, with varied structural parameters dependent on D. Magnetization (M) measurements indicated a considerable difference between zero-field-cooled and field-cooled magnetizations at temperatures below ferromagnetic-paramagnetic (FM-PM) phase transition, particularly for the samples with D = 25-40 nm. These results are ascribed to spin-glass-like behaviors and magnetic inhomogeneity. We also found the possibility of tuning the FM-PM phase transition temperature (TC) from 77 to 262 K, which is dependent on both D and W (the eg-electron bandwidth). Under an applied field of H = 50 kOe, the absolute maximum magnetic entropy change that achieved around TC can be improved from 4.02 J kg-1 K-1 for D = 40 nm to 6.36 Jṡ kg-1ṡ K-1 for D = 100 nm, corresponding to the relative-cooling-power values of 241-245 Jṡ kg-1. We also analyzed the data of M and magnetic entropy change based on theoretical models to further understand the magnetic property and phase-transition type of the NP samples.

  11. Magnetocaloric effect in In doped YbMnO{sub 3}

    Energy Technology Data Exchange (ETDEWEB)

    Sattibabu, Bhumireddi, E-mail: bsb.satti@gmail.com [School of Engineering Sciences and Technology, University of Hyderabad, Hyderabad 500046 (India); Department of Electronics and Physics, Institute of Science, GITAM University, Visakhapatnam 530045 (India); Bhatnagar, A.K., E-mail: anilb42@gmail.com [School of Physics, University of Hyderabad, Hyderabad 500046 (India); Vinod, K.; Mani, Awadhesh [Condensed Matter Physics Division, Materials Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102 (India)

    2017-06-01

    Magnetic and magnetocaloric (MCE) properties of Yb{sub 0.9}In{sub 0.1}MnO{sub 3} and Yb{sub 0.8}In{sub 0.2}MnO{sub 3} polycrystalline samples are presented in this paper. Isothermal magnetization measurements reveal a field induced magnetic transition. Magnetic entropy change of 2.34±0.35 J/mole-K for Yb{sub 0.9}In{sub 0.1}MnO{sub 3} and 2.64±0.38 J/mole-K for Yb{sub 0.8}In{sub 0.2}MnO{sub 3} field change ΔH =10 KOe is observed around the ferromagnetic ordering temperature of Yb{sup 3+}. Values of relative cooling power for the same field change are found to be 38.03±9 J /mol, and 40.90±10 J/mol for Yb{sub 0.9}In{sub 0.1}MnO{sub 3} and Yb{sub 0.8}In{sub 0.2}MnO{sub 3}, respectively. These values suggest In doped YbMnO{sub 3} may be a potential candidate for magnetic refrigerant at low temperatures.

  12. Table-like magnetocaloric effect in Gd56Ni15Al27Zr2 alloy and its field independence feature

    International Nuclear Information System (INIS)

    Agurgo Balfour, E.; Ma, Z.; Fu, H.; Wang, L.; Luo, Y.; Hadimani, R. L.; Jiles, D. C.; Wang, S. F.

    2015-01-01

    In order to obtain “table-like” magnetocaloric effect (MCE), multiple-phase Gd 56 Ni 15 Al 27 Zr 2 alloy was prepared by arc-melting followed by suck-casting method. Powder x-ray diffraction and calorimetric measurements reveal that the sample contains both glassy and crystalline phases. The fraction of the glassy phase is about 62%, estimated from the heat enthalpy of the crystallization. The crystalline phases, Gd 2 Al and GdNiAl further broadened the relatively wider magnetic entropy change (−ΔS M ) peak of the amorphous phase, which resulted in the table-like MCE over a maximum temperature range of 52.5 K to 77.5 K. The plateau feature of the MCE was found to be nearly independent of the applied magnetic field from 3 T to 5 T. The maximum −ΔS M value of the MCE platforms is 6.0 J/kg K under applied magnetic field change of 5 T. Below 3 T, the field independence of the table-like feature disappears. The relatively large constant values of −ΔS M for the respective applied magnetic fields have promising applications in magnetic refrigeration using regenerative Ericsson cycle

  13. A Gallium-Based Magnetocaloric Liquid Metal Ferrofluid.

    Science.gov (United States)

    A de Castro, Isabela; Chrimes, Adam F; Zavabeti, Ali; Berean, Kyle J; Carey, Benjamin J; Zhuang, Jincheng; Du, Yi; Dou, Shi X; Suzuki, Kiyonori; Shanks, Robert A; Nixon-Luke, Reece; Bryant, Gary; Khoshmanesh, Khashayar; Kalantar-Zadeh, Kourosh; Daeneke, Torben

    2017-12-13

    We demonstrate a magnetocaloric ferrofluid based on a gadolinium saturated liquid metal matrix, using a gallium-based liquid metal alloy as the solvent and suspension medium. The material is liquid at room temperature, while exhibiting spontaneous magnetization and a large magnetocaloric effect. The magnetic properties were attributed to the formation of gadolinium nanoparticles suspended within the liquid gallium alloy, which acts as a reaction solvent during the nanoparticle synthesis. High nanoparticle weight fractions exceeding 2% could be suspended within the liquid metal matrix. The liquid metal ferrofluid shows promise for magnetocaloric cooling due to its high thermal conductivity and its liquid nature. Magnetic and thermoanalytic characterizations reveal that the developed material remains liquid within the temperature window required for domestic refrigeration purposes, which enables future fluidic magnetocaloric devices. Additionally, the observed formation of nanometer-sized metallic particles within the supersaturated liquid metal solution has general implications for chemical synthesis and provides a new synthetic pathway toward metallic nanoparticles based on highly reactive rare earth metals.

  14. Magnetism of a sigma-phase Fe{sub 60}V{sub 40} alloy: Magnetic susceptibilities and magnetocaloric effect studies

    Energy Technology Data Exchange (ETDEWEB)

    Bałanda, Maria [Institute of Nuclear Physics, Polish Academy of Science, PL-31-342 Kraków (Poland); Dubiel, Stanisław M., E-mail: Stanislaw.Dubiel@fis.agh.edu.pl [AGH University of Science and Technology, Faculty of Physics and Applied Computer Science, PL-30-059 Kraków (Poland); Pełka, Robert [Institute of Nuclear Physics, Polish Academy of Science, PL-31-342 Kraków (Poland)

    2017-06-15

    Highlights: • Sigma-phase Fe{sub 60}V{sub 40} alloy was studied by means of AC and DC magnetic susceptibilities. • Re-entrant character of the magnetism has been evidenced. • Curie temperature was found as ∼169 K and the spin-freezing temperature as ∼164 K. • Critical exponents β = 0.6, γ = 1.0 and Δ = 1.6 were determined. • Magnetocaloric effect was investigated. - Abstract: Magnetic properties of a sigma-phase Fe{sub 60}V{sub 40} intermetallic compound were studied by means of ac and dc magnetic susceptibility and magnetocaloric effect measurements. The compound is a soft magnet yet it was found to behave like a re-entrant spin-glass system. The magnetic ordering temperature was found to be T{sub C} ≈ 170 K, while the spin-freezing temperature was ∼164 K. Its relative shift per decade of ac frequency was 0.002, a value smaller than that typical of canonical spin-glasses. Magnetic entropy change, ΔS, in the vicinity of T{sub C} was determined for magnetic field, H, ranging between 5 and 50 kOe. Analysis of ΔS in terms of the power law yielded the critical exponent, n, vs. temperature with the minimum value of 0.75 at T{sub C}, while from the analysis of a relative shift of the maximum value of ΔS with the field a critical exponent Δ = 1.7 was obtained. Based on scaling laws relationships values of other two exponents viz. β = 0.6 and γ = 1 were determined.

  15. Influence of Dy addition on the magnetocaloric effect of La0.67Ca0.33Mn0.9V0.1O3 ceramics

    International Nuclear Information System (INIS)

    Nisha, P.; Savitha Pillai, S.; Suresh, K.G.; Raama Varma, Manoj

    2012-01-01

    The influence of partial substitution of La by Dy on the magnetocaloric response of (La 1-x Dy x ) 0.67 Ca 0.33 Mn 0.9 V 0.1 O 3 , where x=0.03, 0.15 and 0.25 is studied. Rietveld refinement of X-ray diffraction pattern using GSAS method shows that the compounds adopt the orthorhombic structure with Pnma space group. The systematic change in lattice parameters and magnetic phase transition indicates the substitution effect of Dy. From the magnetization isotherms at different temperatures, magnetic entropy change close to their respective transition temperatures (T C ) has been evaluated. The maximum value of entropy change near T C is found to be about 4.8 J/kg K at 187.5 K for LCMVDy 0.03 , 2.45 J/kg K at 107.5 K for LCMVDy 0.15 and 2.15 J/kg K at 92.5 K for LCMVDy 0.25 at 4 T. Dy addition produces a reduction in T C and in magnitude of the magnetic entropy change. Even though the entropy change decreases with increasing Dy substitution the refrigerant temperature range, ΔT, is found to be 10 K for LCMVDy 0.03 , 31 K for LCMVDy 0.15 and 35 K for LCMVDy 0.25 compounds [90%] at 4 T. The field dependence of the magnetic entropy change is also analyzed showing the power law dependence, ΔS M ∞H n where n=0.75(2) for LCMVDy 0.03 , n=0.80(4) for LCMVDy 0.15 and n=0.92(8) for LCMVDy 0.25 compounds at their respective transition temperatures. The relative cooling power and its field dependance are also analyzed. - Highlights: → Studied magnetocaloric response of Dy substituted solid state synthesized LCMVO. → Studied the field dependence of the magnetic entropy change (ΔS M ∞H n ). → Studied the field dependence of Relative cooling power (RCP∞H 1+1/δ ). → Considerably large magnetocaloric effect and moderate relative cooling power.

  16. New aspects of magnetocaloric effect in NiMn{sub 0.89}Cr{sub 0.11}Ge

    Energy Technology Data Exchange (ETDEWEB)

    Jaworska-Gołąb, T., E-mail: teresa.jaworska-golab@uj.edu.pl [Institute of Physics, Jagiellonian University, Łojasiewicza 11, 30-348 Kraków (Poland); Baran, S. [Institute of Physics, Jagiellonian University, Łojasiewicza 11, 30-348 Kraków (Poland); Duraj, R. [Institute of Physics, Cracow University of Technology, Podchorążych 1, 30-084 Kraków (Poland); Marzec, M. [Institute of Physics, Jagiellonian University, Łojasiewicza 11, 30-348 Kraków (Poland); Dyakonov, V. [Institute of Physics, Polish Academy of Sciences, al. Lotników 32/46, 02-668 Warszawa (Poland); A.A. Galkin Donetsk Physico-Technical Institute, 83-114 Donetsk (Ukraine); Sivachenko, A. [A.A. Galkin Donetsk Physico-Technical Institute, 83-114 Donetsk (Ukraine); Tyvanchuk, Yu. [Chemistry Department, Ivan Franko National University of Lviv, 79-005 Lviv (Ukraine); Szymczak, H. [Institute of Physics, Polish Academy of Sciences, al. Lotników 32/46, 02-668 Warszawa (Poland); Szytuła, A. [Institute of Physics, Jagiellonian University, Łojasiewicza 11, 30-348 Kraków (Poland)

    2015-07-01

    Investigations of structural and magnetic phase transitions in the NiMn{sub 0.89}Cr{sub 0.11}Ge half-Heusler alloy were carried out by DSC, XRD (80–400 K), magnetic susceptibility and magnetization (1.9–400 K, magnetic field up to 9.0 T, pressure up to 5.25 kbar) measurements. At high temperatures the sample is a single phase crystallizing in the hexagonal crystal structure (Ni{sub 2}In-type, space group P6{sub 3}/mmc) while below 260 K, down to 100 K, some amount of the hexagonal phase coexists with the orthorhombic (TiNiSi-type, space group Pnma) one. Strong magnetostructural coupling is observed. Magnetic data indicate that with increasing temperature magnetic properties of the sample change from antiferro- to ferro- and then to paramagnetic ones. The latter magnetic phase transition is associated with the crystal structure change and results in large magnetic entropy change equal to −51 J/kg K at μ{sub 0}H= 9.0 T near 260 K. Application of external pressure shifts T{sub C} towards lower temperatures. - Highlights: • # Pnma below 210 K, # P6{sub 3}/mmc above 260 K, for 210 K magnetocaloric effect observed about 260 K at ambient pressure. • Magnetostructural effect observed at 260 K (ΔV/V= 2.4%) at ambient pressure. • Magnetic measurements under hydrostatic pressure up to 5.25 kbar; (p, T) diagram.

  17. Insulating phase in Sr{sub 2}IrO{sub 4}: An investigation using critical analysis and magnetocaloric effect

    Energy Technology Data Exchange (ETDEWEB)

    Bhatti, Imtiaz Noor; Pramanik, A.K., E-mail: akpramanik@mail.jnu.ac.in

    2017-01-15

    The nature of insulating phase in 5d based Sr{sub 2}IrO{sub 4} is quite debated as the theoretical as well as experimental investigations have put forward evidences in favor of both magnetically driven Slater-type and interaction driven Mott-type insulator. To understand this insulating behavior, we have investigated the nature of magnetic state in Sr{sub 2}IrO{sub 4} through studying critical exponents, low temperature thermal demagnetization and magnetocaloric effect. The estimated critical exponents do not exactly match with any universality class, however, the values obey the scaling behavior. The exponent values suggest that spin interaction in present material is close to mean-field model. The analysis of low temperature thermal demagnetization data, however, shows dual presence of localized- and itinerant-type of magnetic interaction. Moreover, field dependent change in magnetic entropy indicates magnetic interaction is close to mean-field type. While this material shows an insulating behavior across the magnetic transition, yet a distinct change in slope in resistivity is observed around T{sub c}. We infer that though the insulating phase in Sr{sub 2}IrO{sub 4} is more close to be Slater-type but the simultaneous presence of both Slater- and Mott-type is the likely scenario for this material. - Highlights: • Critical analysis shows Sr{sub 2}IrO{sub 4} has ferromagnetic ordering temperature T{sub c}~225 K. • Obtained critical exponents imply spin interaction is close to mean-field model. • Analysis of magneto-entropy data also supports mean-field type interaction. • However, the presence of both itinerant and localized spin interaction is evident. • Sr{sub 2}IrO{sub 4} has simultaneous presence of both Slater- and Mott-type insulating phase.

  18. Magnetocaloric effect in (La1-xAx)2/3Ba1/3Mn1.05O3-δ

    DEFF Research Database (Denmark)

    Ancona-Torres, Carlos Eugenio; Menon, Mohan; Bahl, Christian Robert Haffenden

    Recently, a large magnetocaloric effect has been reported in La2/3Ba1/3MnO3-δ at about 300 K. In this paper, we investigate the effect of the ion size distribution at the A site on the magnetocaloric effect of this perovskite material. This is accomplished by replacing the lanthanum by Ce, Pr......, and Nd, which allows us to study the effect of both the average size, , and the distribution, σrA, on the magnetic properties of the system. Using magnetization and heat capacity measurements, we determine the important magnetocaloric parameters ΔSM and ΔTad of (La1-xAx)2/3Ba1/3Mn1.05O3-δ powders...

  19. Inverse magnetocaloric effect in Mn2NiGa and Mn1.75Ni1.25Ga magnetic shape memory alloys

    International Nuclear Information System (INIS)

    Singh, Sanjay; Barman, S. R.; Esakki Muthu, S.; Arumugam, S.; Senyshyn, A.; Rajput, P.; Suard, E.

    2014-01-01

    Inverse magnetocaloric effect is demonstrated in Mn 2 NiGa and Mn 1.75 Ni 1.25 Ga magnetic shape memory alloys. The entropy change at the martensite transition is larger in Mn 1.75 Ni 1.25 Ga, and it increases linearly with magnetic field in both the specimens. Existence of inverse magnetocaloric effect is consistent with the observation that magnetization in the martensite phase is smaller than the austenite phase. Although the Mn content is smaller in Mn 1.75 Ni 1.25 Ga, from neutron diffraction, we show that the origin of inverse magnetocaloric effect is the antiferromagnetic interaction between the Mn atoms occupying inequivalent sites

  20. The influence of hysteresis on the determination of the magnetocaloric effect in Gd5Si2Ge2

    DEFF Research Database (Denmark)

    von Moos, Lars; Bahl, Christian; Nielsen, Kaspar Kirstein

    2015-01-01

    and modelling magnetocaloric materials. It is shown that the model reproduces the magnetization data, directly measured adiabatic temperature changes and provides a good description of the material behavior under application conditions. We find that the material settles in an area of metastability under...

  1. Table-like magnetocaloric effect in Gd–Ni–Al amorphous/nanocrystalline composites

    International Nuclear Information System (INIS)

    Zheng, Qiang; Zhang, Linlin; Du, Juan

    2017-01-01

    In this work, Gd–Ni–Al amorphous/nanocrystalline composites produced by melt-spinning method with double magnetocaloric effect (MCE) plateaus have been developed. Two MCE plateaus, ∼4.7 J kg −1 K −1 (90–120 K) and ∼3.60 J kg −1 K −1 (250–275 K), were discovered in Gd 80 Ni 11.6 Al 8.4 for a magnetic field change of 0 to 5 T. For Gd 90 Ni 5.8 Al 4.2 , the plateau values are ∼3.90 J kg −1 K −1 (85–120 K) and ∼6.70 J kg −1 K −1 (265–280 K) for a magnetic field change of 0–5 T. The reason why MCE plateau formation was investigated and discussed. These composites having two MCE plateaus are competitive candidates for the ideal Ericsson cycle. (paper)

  2. Strain dependent magnetocaloric effect in La0.67Sr0.33MnO3 thin-films

    Directory of Open Access Journals (Sweden)

    V. Suresh Kumar

    2013-05-01

    Full Text Available The strain dependent magnetocaloric properties of La0.67Sr0.33MnO3 thin films deposited on three different substrates (001 LaAlO3 (LAO, (001 SrTiO3 (STO, and (001 La0.3Sr0.7Al0.65Ta0.35O9 (LSAT have been investigated under low magnetic fields and around magnetic phase transition temperatures. Compared to bulk samples, we observe a remarkable decrease in the ferromagnetic transition temperature that is close to room temperature, closely matched isothermal magnetic entropy change and relative cooling power values in tensile strained La0.67Sr0.33MnO3 films. The epitaxial strain plays a significant role in tuning the peak position of isothermal magnetic entropy change towards room temperature with improved cooling capacity.

  3. Study of multi-layer active magnetic regenerators using magnetocaloric materials with first and second order phase transition

    DEFF Research Database (Denmark)

    Lei, Tian; Engelbrecht, Kurt; Nielsen, Kaspar Kirstein

    2016-01-01

    Magnetocaloric materials (MCM) with a first order phase transition (FOPT) usually exhibit a large, although sharp, isothermal entropy change near their Curie temperature, compared to materials with a second order phase transition (SOPT). Experimental results of applying FOPT materials in recent...... magnetocaloric refrigerators (MCR) demonstrated the great potential for these materials, but a thorough study on the impact of the moderate adiabatic temperature change and strong temperature dependence of the magnetocaloric effect (MCE) is lacking. Besides, comparing active magnetic regenerators (AMR) using...... FOPT and SOPT materials is also of fundamental interest. We present modeling results of multi-layer AMRs using FOPT and SOPT materials based on a 1D numerical model. First the impact of isothermal entropy change, adiabatic temperature change and shape factor describing the temperature dependence...

  4. Scaling and universality in magnetocaloric materials

    DEFF Research Database (Denmark)

    Smith, Anders; Nielsen, Kaspar Kirstein; Bahl, Christian R. H.

    2014-01-01

    -order phase transition within the context of the theory of critical phenomena. Sufficiently close to the critical temperature of a second-order material, the scaling of the isothermal entropy change will be determined by the critical exponents and will be the same as that of the singular part of the entropy......The magnetocaloric effect of a magnetic material is characterized by two quantities, the isothermal entropy change and the adiabatic temperature change, both of which are functions of temperature and applied magnetic field. We discuss the scaling properties of these quantities close to a second...... fields are not universal, showing significant variation for models in the same universality class. As regards the adiabatic temperature change, it is not determined exclusively by the singular part of the free energy and its derivatives. We show that the field dependence of the adiabatic temperature...

  5. Enhanced magnetocaloric properties and critical behavior of (Fe0.72Cr0.28)3Al alloys for near room temperature cooling

    Science.gov (United States)

    Sharma, V.; Maheshwar Repaka, D. V.; Chaudhary, V.; Ramanujan, R. V.

    2017-04-01

    Magnetic cooling is an environmentally friendly, energy efficient, thermal management technology relying on high performance magnetocaloric materials (MCM). Current research has focused on low cost, corrosion resistant, rare earth (RE) free MCMs. We report the structural and magnetocaloric properties of novel, low cost, RE free, iron based (Fe0.72Cr0.28)3Al alloys. The arc melted buttons and melt spun ribbons possessed the L21 crystal structure and B2 crystal structure, respectively. A notable enhancement of 33% in isothermal entropy change (-ΔS m) and 25% increase in relative cooling power (RCP) for the ribbons compared to the buttons can be attributed to higher structural disorder in the Fe-Cr and Fe-Al sub-lattices of the B2 structure. The critical behavior was investigated using modified Arrott plots, the Kouvel-Fisher plot and the critical isotherm technique; the critical exponents were found to correspond to the short-range order 3D Heisenberg model. The field and temperature dependent magnetization curves of (Fe0.72Cr0.28)3Al alloys revealed their soft magnetic nature with negligible hysteresis. Thus, these alloys possess promising performance attributes for near room temperature magnetic cooling applications.

  6. Magnetocaloric properties and critical behavior of high relative cooling power FeNiB nanoparticles

    Science.gov (United States)

    Chaudhary, V.; Maheswar Repaka, D. V.; Chaturvedi, A.; Sridhar, I.; Ramanujan, R. V.

    2014-10-01

    Low cost magnetocaloric nanomaterials have attracted considerable attention for energy efficient applications. We report a very high relative cooling power (RCP) in a study of the magnetocaloric effect in quenched FeNiB nanoparticles. RCP increases from 89.8 to 640 J kg-1 for a field change of 1 and 5 T, respectively, these values are the largest for rare earth free iron based magnetocaloric nanomaterials. To investigate the magnetocaloric behavior around the Curie temperature (TC), the critical behavior of these quenched nanoparticles was studied. Detailed analysis of the magnetic phase transition using the modified Arrott plot, Kouvel-Fisher method, and critical isotherm plots yields critical exponents of β = 0.364, γ = 1.319, δ = 4.623, and α = -0.055, which are close to the theoretical exponents obtained from the 3D-Heisenberg model. Our results indicate that these FeNiB nanoparticles are potential candidates for magnetocaloric fluid based heat pumps and low grade waste heat recovery.

  7. In-situ neutron investigation of hydrogen absorption kinetics in La(FexSi1-x)13 magnetocaloric alloys for room-temperature refrigeration application

    Science.gov (United States)

    Hai, Xueying; Mayer, Charlotte; Colin, Claire V.; Miraglia, Salvatore

    2016-02-01

    Promising magnetocaloric material La(Fe,Si)13 with a first-order magnetic transition has been widely investigated. The observed instability of hydrogen in the material is detrimental for its industrial upscale and a better control of the hydrogen absorption/desorption is necessary to optimize its application potential. In this article, the hydrogen absorption kinetics is studied through an in-situ neutron diffraction experiment. The results allow us to have an inside look at the structure "breathing" to accommodate the interstitial atoms and compare the effect of hydrides with carbohydrides.

  8. The effect of adding aluminum and iron to Tb–Dy–Ho–Co multicomponent alloys on their structure and magnetic and magnetocaloric properties

    Czech Academy of Sciences Publication Activity Database

    Politova, G.A.; Burkhanov, G.S.; Tereshina, I. S.; Kaminskaya, T.; Chzhan, V.B.; Tereshina, Evgeniya

    2017-01-01

    Roč. 62, č. 4 (2017), s. 577-582 ISSN 1063-7842 Institutional support: RVO:68378271 Keywords : multicomponent alloys * Laves phase compounds * magnetocaloric effect Subject RIV: BM - Solid Matter Physics ; Magnetism OBOR OECD: Condensed matter physics (including formerly solid state physics, supercond.) Impact factor: 0.632, year: 2016

  9. Pressure enhancement of the giant magnetocaloric effect in Tb.sub.5./sub.Si.sub.2./sub.Ge.sub.2./sub..

    Czech Academy of Sciences Publication Activity Database

    Morellon, L.; Arnold, Zdeněk; Magen, C.; Ritter, C.; Skorokhod, Yuriy; Prokhnenko, Olexandr; Algarabel, P. A.; Ibarra, M. R.; Kamarád, Jiří

    2004-01-01

    Roč. 93, č. 13 (2004), 137201/1-137201/4 ISSN 0031-9007 R&D Projects: GA ČR GA106/02/0943 Institutional research plan: CEZ:AV0Z1010914 Keywords : magnetocaloric effect * high-pressure * neutron diffraction Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 7.218, year: 2004

  10. Magnetocaloric effect of Gd.sub.64./sub.Co.sub.26./sub.Al.sub.9./sub.Y.sub.1./sub. metallic glass

    Czech Academy of Sciences Publication Activity Database

    Kaštil, J.; Kamarád, Jiří; Javorský, P.

    2012-01-01

    Roč. 545, Dec (2012), s. 1-4 ISSN 0925-8388 R&D Projects: GA ČR GAP204/12/0692; GA ČR GD202/09/H041 Institutional support: RVO:68378271 Keywords : BMG * magnetocaloric effect * magnetism Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 2.390, year: 2012

  11. Influence of structural defects on the magnetocaloric effect in the vicinity of the first order magnetic transition in Fe50.4Rh49.6

    Science.gov (United States)

    Zverev, V. I.; Saletsky, A. M.; Gimaev, R. R.; Tishin, A. M.; Miyanaga, T.; Staunton, J. B.

    2016-05-01

    The large magnetocaloric effect (MCE), which accompanies the first order ferromagnetic/anti-ferromagnetic transition in CsCl-ordered Fe-Rh alloys, has been investigated by measurements in slowly cycled magnetic fields of up to 2 T in magnitude for a range of temperatures, 300 K < T < 350 K. A bulk sample with composition Fe50.4Rh49.6 was used and the results were compared with those produced by the ab-initio density functional theory-based disordered local moment theory of the MCE. The measurements revealed an irreversibility effect in which the temperature of the material did not return to its initial value following several cycles of the magnetic field. These observations were explained in the framework of the ab-initio theory for the first order transition in which the consequences of the incomplete long range compositional order and small compositional inhomogeneities of the sample were included. The mean value of the long range order parameter S used in the theoretical work was 0.985, close to the value obtained experimentally from XRD measurements. The sample inhomogeneities were modeled by regions in the sample having a distribution of S values with narrow half-width 0.004 about the mean value. The influence of such compositional disorder on both the transition temperature (323.5 K) and MCE adiabatic temperature change (ΔT = 7.5 K) was also studied.

  12. Spin correlations in (Mn,Fe2(P,Si magnetocaloric compounds above Curie temperature

    Directory of Open Access Journals (Sweden)

    X.F. Miao

    2016-06-01

    Full Text Available The longitudinal-field muon-spin relaxation (LF-μSR technique was employed to study the spin correlations in (Mn,Fe2(P,Si compounds above the ferromagnetic transition temperature (TC. The (Mn,Fe2(P,Si compound under study is found to show itinerant magnetism. The standard deviation of the magnetic field distribution of electronic origin increases with a decrease in temperature, which is attributed to the development of spin correlations. The anomalously low magnetic fluctuation rate is suggested to be another signature of the spin correlations. The development of pronounced magnetic fluctuations is in agreement with the observed deviation of the paramagnetic susceptibility from Curie–Weiss behavior. Our study sheds light on the magneto-elastic transition and the mixed magnetism in (Mn,Fe2(P,Si compounds.

  13. CONDENSED MATTER: ELECTRONIC STRUCTURE, ELECTRICAL, MAGNETIC, AND OPTICAL PROPERTIES: Magnetic properties and magnetocaloric effect in Ndx La1-x Fe11.5 Al1.5 compounds

    Science.gov (United States)

    Wang, Fang; Wang, Guang-Jun; Sun, Ji-Rong; Shen, Bao-Gen

    2008-08-01

    Effects of Nd-doping on the magnetic properties and magnetocaloric effects (MCEs) of NdxLa1-x Fe11.5 Al1.5 have been investigated. Substitution of Nd leads to a weakening of the antiferromagnetic (AFM) coupling and an enhancement of the ferromagnetic (FM) coupling. This in turn results in a complex magnetic behaviour for Nd0.2La0.8Fe11.5Al1.5 characterized by the occurrence of two phase transitions at ~188K (PM-AFM) and ~159K (AFM-FM). As a result, a table-like MCE (9 J/kg·K) is found in a wide temperature range (160-185 K) for a field change of 0-5T around the transition temperature, as evidenced by both the magnetic and calorimetric measurements. Based on the analysis of low-temperature heat capacity, it is found that the AFM-FM phase transition modifies the electron density significantly, and the major contribution to the entropy change comes from the electronic entropy change.

  14. Theoretical investigations on magnetocaloric effect in Er{sub 1−y}Tb{sub y}Al{sub 2} series

    Energy Technology Data Exchange (ETDEWEB)

    Ribeiro, P.O., E-mail: paula.ribeiro@gmail.com [Instituto de Física, Universidade do Estado do Rio de Janeiro – UERJ, Rua São Francisco Xavier, 524, 20550-013 RJ (Brazil); Alho, B.P.; Alvarenga, T.S.T.; Nóbrega, E.P.; Sousa, V.S.R. de [Instituto de Física, Universidade do Estado do Rio de Janeiro – UERJ, Rua São Francisco Xavier, 524, 20550-013 RJ (Brazil); Carvalho, A. Magnus G. [Laboratório Nacional de Luz Síncrotron, CNPEM, 13083-970 Campinas, SP (Brazil); Caldas, A. [Sociedade Unificada de Ensino Superior e Cultura, SUESC, 20211-351 Rio de Janeiro, RJ (Brazil); Oliveira, N.A. de; Ranke, P.J. von [Instituto de Física, Universidade do Estado do Rio de Janeiro – UERJ, Rua São Francisco Xavier, 524, 20550-013 RJ (Brazil)

    2015-04-01

    We report on the magnetic and magnetocaloric effect calculations in rare earth Er{sub 1−y}Tb{sub y}Al{sub 2} compounds (y=0.00, 0.25, 0.5, 0.75 and 1.00). Our model Hamiltonian has contributions of the crystalline electrical field anisotropy in both Er and Tb magnetic sublattices, disorder in exchange interactions among Er–Er, Tb–Tb and Er–Tb magnetic ions and the Zeeman effect. The magnetization, the isothermal entropy change (ΔS{sub T}) and the adiabatic temperature change (ΔT{sub ad}) dependence on temperature were simulated and, compared with the experimental data available. - Highlights: • Modeling Er{sub (1−y)}Tb{sub y}Al{sub 2} intermetallic compounds. • Magnetic entropy changes in Er{sub (1−y)}Tb{sub y}Al{sub 2}. • Adiabatic temperature changes in Er{sub 0.75}Tb{sub 0.25}Al{sub 2} and Er{sub 0.65}Tb{sub 0.35}Al{sub 2} compounds.

  15. Magnetocaloric effect in materials with the first order transitions - direct measurements

    Czech Academy of Sciences Publication Activity Database

    Kamarád, Jiří; Kaštil, J.; Arnold, Zdeněk; Javorský, P.; Sechovský, V.

    2010-01-01

    Roč. 118, č. 5 (2010), s. 1000-1001 ISSN 0587-4246 R&D Projects: GA ČR GA202/09/0030 Grant - others:GA ČR(CZ) GA101/07/1173 Institutional research plan: CEZ:AV0Z10100521 Keywords : magneto-caloric characteristics * first order transitions * Gd Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 0.467, year: 2010 http://przyrbwn.icm.edu.pl/APP/PDF/118/a118z5p117.pdf

  16. The magnetocaloric effect and the heat capacity of aqueous suspensions of porphyrin complexes of rare earth elements according to microcalorimetric data

    Science.gov (United States)

    Korolev, V. V.; Korolev, D. V.; Lomova, T. N.; Mozhzhukhina, E. G.; Zakharov, A. G.

    2012-03-01

    The magnetocaloric effect (MCE) and heat capacity during the magnetization process of (5,10,15,20-tetraphenylporphyrinato)acetatogadolinium(III), (AcO)GdTPP, and (5,10,15,20-tetraphenylporphyrinato)chlorogadolinium(III) complexes, (Cl)GdTPP, in the form of 6%-aqeous suspensions are determined by the microcalorimetric method in a range of temperatures from 278 to 318 K and magnetic fields from 0 to 1 T. It is found that MCE for all the complexes are positive, i.e., at applying a magnetic field in the adiabatic conditions temperature of a suspension of complex increases. It is established that MCE increases with an increase in magnetic induction at all temperatures and decreases with an increase in temperature at all magnetic fields. It is shown that the substitution of chloride ligand by acetate in (X)GdTPP leads to a significant increas in MCE and its temperature dependence; in the case of (Cl)GdTPP actually MCE does not depend on temperature. Relationships between magnetothermal properties and structure of the complexes are analyzed. The conclusion is argumented that the reason of changes in magnetothermal properties after the replacement of axial ligand in gadolinium complexes and complexes of lanthanides with an unsymmetrically filled f-shell is non-planar geometry of the coordination site and specific electronic properties of the central ion. It is concluded that heat capacity of the complexes slightly increases with an increase in temperature and more noticeably in the case of (AcO)GdTPP; a magnetic component of heat capacity is revealed only in (AcO)GdTPP at temperatures above 298 K, which is connected perhaps with a temperature change in the crystal lattice of the complex and influence of the magnetic properties of gadolinium ion on this change.

  17. Evolution of magnetostructural transition and magnetocaloric effect with Al doping in MnCoGe1-xAlx compounds

    KAUST Repository

    Bao, Lifu

    2014-01-03

    The effect of Al doping in MnCoGe1-xAlx compounds has been investigated. The substitution of Al for Ge enhances Mn-Mn covalent bonding by shortening the distance of nearest Mn atom layers, and thus stabilizes the hexagonal structure. As a result, first-order magnetostructural transition between ferromagnetic martensite and paramagnetic austenite takes place for the optimized compositions (x = 0.01, 0.02). Accompanied with the magnetostructural transition, large magnetocaloric effect (MCE) is observed. More doping of Al(x = 0.03, 0.04) leads to the separation of magnetic and structural transitions and remarkable reduction of MCE. © 2014 IOP Publishing Ltd.

  18. Microstructure evolution and large magnetocaloric effect of La0.8Ce0.2(Fe0.95Co0.05)11.8Si1.2 alloy prepared by strip-casting and annealing

    Science.gov (United States)

    Zhong, X. C.; Feng, X. L.; Huang, J. H.; Zhang, H.; Huang, Y. L.; Liu, Z. W.; Jiao, D. L.

    2018-04-01

    The microstructure and magnetocaloric effect of the La0.8Ce0.2(Fe0.95Co0.05)11.8Si1.2 strip-cast flakes annealed between 1273K and 1423K for different time have been investigated. For the flakes annealed for 2h from 1273K to 1423K, the shape and distribution of α-Fe, La-rich and NaZn13-type 1:13 phases are quite sensitive to the annealing temperature. Especially, at a high annealing temperature of 1423K, the 1:13 phase began to decompose into macroscopic α-Fe conglomerations and La-rich dendrites. With the increase of annealing time from 0 to 12h at 1323K, the amount of 1:13 phase increased significantly and reached ˜93.50 wt.% at 12h. However, an overlong annealing time also led to 1:13 phase decomposition and influenced the magnetic performance. For the flakes annealed at 1323K for 12h, large magnetic entropy change value of 18.12Jkg-1K-1 at 5T has been obtained. The present results indicate that strip casting method can potentially be used in mass production of high performance magnetocaloric materials.

  19. Magneto-thermal conduction and magneto-caloric effect in poly and nano crystalline forms of multiferroic GdCrO3

    International Nuclear Information System (INIS)

    Uma, S; Philip, J

    2014-01-01

    Gadolinium chromite, GdCrO 3 , belongs to the family of rare earth chromites, exhibiting multiferroism with coupling between electric polarization and magnetic ordering. It is understood that the interaction between Gd 3+ and Cr 3+ ions is responsible for switchable polarization in this system. Below Néel temperature the spins of Cr 3+ ions interact in anti-parallel through super exchange mechanism, giving rise to antiferromagnetic ordering at around 169 K in poly and nanocrystalline phases of this material. In order to understand the nature of spin–lattice coupling and magnon–phonon interaction in the intermediate temperature range (150–250 K), the magneto-thermal conduction and magneto-caloric effect in poly and nanocrystalline forms of this material are reported. These properties show anomalies around 169 K, which is described as due to spin–phonon coupling. When particle sizes are reduced to nanometer scales, thermal conductivity decreases significantly while specific heat capacity increases. The former is explained as due to reduction in phonon mean free path and phonon scattering from nanoparticle interfaces, while the latter is ascribed to contributions from Einstein oscillators at weakly bound atoms at the interfaces of nanocrystals. (paper)

  20. Effects of the partial substitution of Ni by Cr on the transport, magnetic, and magnetocaloric properties of Ni50Mn37In13

    Directory of Open Access Journals (Sweden)

    Sudip Pandey

    2017-05-01

    Full Text Available The structural, magnetic, and magnetotransport properties of Ni50-xCrxMn37In13 Heusler alloys have been synthesized and investigated by x-ray diffraction (XRD, field and pressure dependent magnetization, and electrical resistivity measurements. The partial substitution of Ni by Cr in Ni50Mn37In13 significantly improves the magnetocaloric effect in the vicinity of the martensitic transition (TM. This system also shows a large negative entropy change at the Curie temperature (TC, making it a candidate material for application in a refrigeration cycle that exploits both positive and negative magnetic entropy changes. The refrigeration capacity (RC values at TM and TC increase significantly by more than 20 % with Cr substitution. The application of hydrostatic pressure increases the temperature stability of the martensitic phase in Ni45Cr5Mn37In13. The influence of Cr substitution on the transport properties of Ni48Cr2Mn37In13 is discussed. An asymmetric magnetoresistance, i.e., a spin-valve-like behavior, has been observed near TM for Ni48Cr2Mn37In13.

  1. Operational test of bonded magnetocaloric plates

    DEFF Research Database (Denmark)

    Bahl, Christian; Navickaité, Kristina; Neves Bez, Henrique

    2017-01-01

    Bonded plates made by hot pressing La0.85Ce0.15Fe11.25Mn0.25Si1.5Hy particles and resin have been tested as active magnetic regenerators in a small scale magnetocaloric device. Firstly the plates were carefully characterised magnetically and thermally. The plates were prepared with 5 wt% resin......, and from density measurements it was found that the volume ratio of the magnetocaloric material in the plates was 0.53, due to the resin and porosity. The best operating conditions for the plate regenerator were determined at which a temperature span of 6.4 K was measured along the plates....

  2. Analysis of the Magnetocaloric Effect in Heusler Alloys: Study of Ni50CoMn36Sn13 by Calorimetric Techniques

    Directory of Open Access Journals (Sweden)

    Elias Palacios

    2015-03-01

    Full Text Available Direct determinations of the isothermal entropy increment, \\(-\\Delta S_T\\, in the Heusler alloy Ni\\(_{50}\\CoMn\\(_{36}\\Sn\\(_{13}\\ on demagnetization gave positive values, corresponding to a normal magnetocaloric effect. These values contradict the results derived from heat-capacity measurements and also previous results obtained from magnetization measurements, which indicated an inverse magnetocaloric effect, but showing different values depending on the technique employed. The puzzle is solved, and the apparent incompatibilities are quantitatively explained considering the hysteresis, the width of the martensitic transition and the detailed protocol followed to obtain each datum. The results show that these factors should be analyzed in detail when dealing with Heusler alloys.

  3. Pressure effects in the giant magnetocaloric compounds Gd.sub.5./sub.(Si.sub.x./sub.Ge.sub.1 - x./sub.).sub.4./sub..

    Czech Academy of Sciences Publication Activity Database

    Morellon, L.; Arnold, Zdeněk; Algarabel, P. A.; Magen, C.; Ibarra, M. R.; Skorokhod, Yuriy

    2004-01-01

    Roč. 16, - (2004), s. 1623-1630 ISSN 0953-8984 R&D Projects: GA ČR GA106/02/0943 Grant - others:CICYT(ES) MAT2000-1756 Institutional research plan: CEZ:AV0Z1010914 Keywords : magnetocaloric effect * high pressure * Gd 5 Si 4-x Ge x * magnetic transitions Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 2.049, year: 2004

  4. High performance magnetocaloric perovskites for magnetic refrigeration

    DEFF Research Database (Denmark)

    Bahl, Christian R. H.; Velazquez, David; Nielsen, Kaspar K.

    2012-01-01

    We have applied mixed valance manganite perovskites as magnetocaloric materials in a magnetic refrigeration device. Relying on exact control of the composition and a technique to process the materials into single adjoined pieces, we have observed temperature spans above 9 K with two materials...

  5. Large rotating magnetocaloric effect in ErAlO3 single crystal

    Directory of Open Access Journals (Sweden)

    X. Q. Zhang

    2017-05-01

    Full Text Available Magnetic and magnetocaloric properties of ErAlO3 single crystal were investigated. Magnetization of ErAlO3 shows obvious anisotropy when magnetic field is applied along the a, b and c axes, which leads to large anisotropic magnetic entropy change. In particular, large rotating field entropy change from the b to c axis within the bc plane is obtained and reaches 9.7 J/kg K at 14 K in a field of 5 T. This suggests the possibility of using ErAlO3 single crystal for magnetic refrigerators by rotating its magnetization vector rather than moving it in and out of the magnet.

  6. Effect of Sm substitution on magnetic and magnetocaloric properties of La0.7-xSmxBa0.3MnO3 (0 ≤ x ≤ 0.2) compounds

    Science.gov (United States)

    Modi, Anchit; Gaur, N. K.

    2017-11-01

    In the present paper we have studied the effect of Sm doping on the magnetic and magnetocaloric properties of La0.7-xSmxBa0.3MnO3 (0 ≤ x ≤ 0.2) compounds. These sample have been synthesized by conventional solid state reaction method. The analysis of synthesized samples by X-ray diffraction showed that the formation of single phase compositions and doping of La3+ by Sm3+ ion converted the chemical structure form rhombohedral (R-3C) to orthorhombic (Imma). The magnetic study measurement specified that the ferromagnetic double exchange interaction is weakened with increasing Sm content as a consequence of the curie temperature (Tc) shift in lower temperature from 340 K for x = 0, 290 K for x = 0.1 and 225 K for x = 0.2 compounds. Using the Banerjee's criterion plots, it is found that the phase transition for all samples in the second-order. All reported compounds exhibit a maximum and large magneto-caloric effect near the Curie temperature (Tc). The magnitude of the maximum magnetic entropy change is found to be decrease with increasing of Sm doping content i.e. 4.39 J/kg K for x = 0, 4.22 J/kg K for x = 0.1 and 2.48 J/kg K for x = 0.2 in applied field change of 5T. The trend of large entropy change and the convenient adjustment of the Curie temperature make these oxides useful for magnetic refrigeration in an extended high and low temperature even at near room temperature.

  7. Table-like magnetocaloric effect in Gd{sub 56}Ni{sub 15}Al{sub 27}Zr{sub 2} alloy and its field independence feature

    Energy Technology Data Exchange (ETDEWEB)

    Agurgo Balfour, E.; Ma, Z.; Fu, H., E-mail: fuhao@uestc.edu.cn, E-mail: rockingsandstorm@163.com; Wang, L.; Luo, Y. [School of Physical Electronics, University of Electronic Science and Technology of China, Chengdu 610054 (China); Hadimani, R. L.; Jiles, D. C. [Department of Electrical and Computer Engineering, Iowa State University, Ames, Iowa 50011 (United States); Ames Laboratory, U.S. Department of Energy, Ames, Iowa 50011 (United States); Wang, S. F., E-mail: fuhao@uestc.edu.cn, E-mail: rockingsandstorm@163.com [North Electronic Device Research Institute, Beijing 100141 (China)

    2015-09-28

    In order to obtain “table-like” magnetocaloric effect (MCE), multiple-phase Gd{sub 56}Ni{sub 15}Al{sub 27}Zr{sub 2} alloy was prepared by arc-melting followed by suck-casting method. Powder x-ray diffraction and calorimetric measurements reveal that the sample contains both glassy and crystalline phases. The fraction of the glassy phase is about 62%, estimated from the heat enthalpy of the crystallization. The crystalline phases, Gd{sub 2}Al and GdNiAl further broadened the relatively wider magnetic entropy change (−ΔS{sub M}) peak of the amorphous phase, which resulted in the table-like MCE over a maximum temperature range of 52.5 K to 77.5 K. The plateau feature of the MCE was found to be nearly independent of the applied magnetic field from 3 T to 5 T. The maximum −ΔS{sub M} value of the MCE platforms is 6.0 J/kg K under applied magnetic field change of 5 T. Below 3 T, the field independence of the table-like feature disappears. The relatively large constant values of −ΔS{sub M} for the respective applied magnetic fields have promising applications in magnetic refrigeration using regenerative Ericsson cycle.

  8. Tuning of normal and inverse magnetocaloric effect in Sm0.35Pr0.15Sr0.5MnO3 phase separated manganites

    International Nuclear Information System (INIS)

    Giri, S.K.; Dasgupta, Papri; Poddar, A.; Nath, T.K.

    2015-01-01

    Graphical abstract: ΔS M vs. T plots of nano (left) and bulk (right) samples at different magnetic fields. - Highlights: • Bulk to nano show first order FM → PM phase transition at low magnetic field. • Bulk sample exhibits normal and inverse MCE around T C and after T g , respectively. • The value of ΔS M at T C is almost three times larger than at T g . • The value of ΔS M also decreases with reduction of particles sizes. • The bulk sample also exhibits a large RCP of 43.5 J/kg for a magnetic field of 1 T. - Abstract: Magnetic and magnetocaloric properties of Sm 0.35 Pr 0.15 Sr 0.5 MnO 3 polycrystalline manganite (bulk and nanometric samples) are investigated in detail. It has been observed that all the particle sizes (bulk to nano) show first order ferromagnetic → paramagnetic phase transition at low magnetic field. Ferromagnetic transition temperature also decreases with decreasing the particle size. This suggests that ferromagnetism is weakened and the first order magnetic phase transition is softened. We have investigated the magnetocaloric effect (MCE) of both bulk and nanometric samples around their spin glass-like transition temperature, T g and Curie temperature, T C . It has been found that bulk sample exhibits both normal (i.e., negative ΔS M ) and inverse (i.e., positive ΔS M ) MCE around T C and after T g , respectively. The value of ΔS M (+3.17 J kg −1 K −1 ) at T C is almost three times larger than at T g (ΔS M = −0.52 J kg −1 K −1 ) for a magnetic field change of 7 T. The bulk sample also exhibits a large relative cooling power (RCP) of 43.5 J/kg for a magnetic field of 1 T. The corresponding adiabatic temperature change of bulk sample is observed to be ∼1.5 K for a magnetic field change of 3 T. The value of ΔS M also decreases with reduction of particles sizes. The temperature width of ΔS M broadens with decreasing particle size. The value of ΔS M and the adiabatic temperature change vary with temperature and it

  9. Effect of Gd substitution on the structural, magnetic, and magnetocaloric properties of HoCrO3

    Science.gov (United States)

    Yin, Shiqi; Zhong, Wei; Guild, Curtis J.; Shi, Jianhang; Suib, Steven L.; Cótica, Luiz Fernando; Jain, Menka

    2018-02-01

    Rare-earth chromites are a new type of magnetoelectric multiferroics. In this work, a Ho0.33Gd0.67CrO3 powder sample was synthesized via a citrate route, and the structural properties were characterized by X-ray diffraction, scanning electron microscopy, and the Raman technique. The UV-Visible optical absorbance spectra were also measured in the wavelength range of 200-800 nm. The valence state of Cr was found to be purely 3+ according to the X-ray photoelectron spectroscopy. The temperature-dependent dielectric constant and loss tangent data measured between the frequencies of 1 kHz and 1 MHz show no anomalies around the magnetic transition temperature of the material. The dc magnetization measurements show that the ordering temperature of Cr3+ ( TNC r) is 155 K for Ho0.33Gd0.67CrO3, which is larger than 140 K for HoCrO3. The positive slope of the Arrott plots from 0 T to 7 T reveals that the antiferromagnetic-paramagnetic phase transition is second-order in nature. At a field of 7 T, the Ho0.33Gd0.67CrO3 sample showed a giant magnetocaloric entropy change, -ΔS, of ˜23.3 J/kg K at 5 K, and a refrigeration capacity of ˜481.2 J/kg, which are much higher than those of pure bulk HoCrO3. This renders this material prospective for magnetic refrigeration in the low temperature (<30 K) range.

  10. Glass formation ability, structure and magnetocaloric effect of a heavy rare-earth bulk metallic glassy Gd{sub 55}Co{sub 20}Fe{sub 5}Al{sub 20} alloy

    Energy Technology Data Exchange (ETDEWEB)

    Jo, C.-L. [Shanghai University, School of Materials Science and Engineering, Yanchang Road 149, Zhabei District, 200072 Shanghai (China)], E-mail: jochollong@163.com; Xia Lei; Ding Ding; Dong Yuanda; Gracien, Ekoko [Shanghai University, School of Materials Science and Engineering, Yanchang Road 149, Zhabei District, 200072 Shanghai (China)

    2008-06-30

    The glass formation ability, the structure and the magnetocaloric effect of the bulk metallic glassy Gd{sub 55}Co{sub 20}Fe{sub 5}Al{sub 20} alloy were investigated. Bulk metallic glassy (BMGs) alloys were prepared by a copper-mold casting method. The glass forming ability and their structure were studied by using X-ray diffraction (XRD) and differential scanning calorimeter (DSC). The XRD analysis revealed that the as-cast cylinder of Gd{sub 55}Co{sub 20}Fe{sub 5}Al{sub 20} alloy showed fully amorphous structure in 2 mm diameter. The DSC revealed that the bulk cylinder of the Gd{sub 55}Co{sub 20}Fe{sub 5}Al{sub 20} alloy showed a distinct glass transition temperature and a relatively wide supercooled liquid region before crystallization. SQUID investigated the magnetic properties and the entropy changes. The Curie temperature of Gd{sub 55}Co{sub 20}Fe{sub 5}Al{sub 20} BMGs alloy was about 130 K, but the maximum magnetic entropy changes(-{delta}S{sub M}) showed at about 125 K, a little lower than the Curie temperature 130 K. The reason could probably be due to the presence of a little amount of nanocrystalline particles between amorphous phases. The BMG alloy has the characteristic of second-order transition (SOT) on Arrott plots. The results showed that the amorphous sample had a relatively improved magnetocaloric effect, indicating that the amorphous alloy could be considered as a candidate for magnetic refrigeration applications in the temperature interval range of 100-200 K.

  11. Magnetic properties and magnetocaloric effect in the R{sub 2}PdSi{sub 3} (R = Gd, Dy and Er) compounds

    Energy Technology Data Exchange (ETDEWEB)

    Mo, Zhao Jun, E-mail: mozhaojun@iphy.ac.cn [School of Material Science and Engineering, Tianjin University of Technology, Tianjin (China); Key Laboratory of Cryogenics, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing (China); Shen, Jun, E-mail: jshen@mail.ipc.ac.cn [Key Laboratory of Cryogenics, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing (China); Gao, Xin Qiang [Key Laboratory of Cryogenics, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing (China); Liu, Yao [State Key Laboratory of Magnetism, Beijing National Laboratory for Condensed Matter, Physics and Institute of Physics, Chinese Academy of Sciences, Beijing (China); Tang, Cheng Chun [School of Material Science and Engineering, Hebei University of Technology, Tianjin (China); Wu, Jian Feng [Key Laboratory of Cryogenics, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing (China); Hu, Feng Xia; Sun, Ji Rong; Shen, Bao Gen [State Key Laboratory of Magnetism, Beijing National Laboratory for Condensed Matter, Physics and Institute of Physics, Chinese Academy of Sciences, Beijing (China)

    2015-03-25

    Highlights: • Er{sub 2}PdSi{sub 3} compound exhibits a giant reversible MCE. • Er{sub 2}PdSi{sub 3} compound’s MCEs show no thermal and magnetic hysteresis. • Under field changes of 2 T, the value of -ΔS{sub M}{sup max} is 14.5 J/kg K and the RC is 111 J/kg, respectively. - Abstract: The magnetic properties and magnetocaloric effect in R{sub 2}PdSi{sub 3} (R = Dy, Dy and Er) compounds have been investigated. All these compounds possess an antiferromagnetic (AFM)-paramagnetic (PM) transition around their respective Néel temperatures. And, it is found that the Dy{sub 2}PdSi{sub 3} and Er{sub 2}PdSi{sub 3} compounds undergo a spin-glass behavior below Néel temperature. Under the magnetic field change of 5 T, the values of -ΔS{sub M}{sup max} reach 11.8 J/kg K for Gd{sub 2}PdSi{sub 3}, 16.6 J/kg K for Dy{sub 2}PdSi{sub 3} and 22 J/kg K for Er{sub 2}PdSi{sub 3}, respectively. Especially, the values of -ΔS{sub M}{sup max} in the Er{sub 2}PdSi{sub 3} compound are 8 and 14.5 J/kg K for field change of 1 and 2 T, which is attributed to a field-induced metamagnetic transition from AFM to FM states. The large reversible -ΔS{sub M} and large RC together with the absence of thermal and field hysteresis indicate that Er{sub 2}PdSi{sub 3} compound could be a promising candidate for magnetic refrigeration at low temperatures.

  12. Magnetic and magnetocaloric properties of martensitic Ni2Mn1.4Sn0.6 Heusler alloy

    International Nuclear Information System (INIS)

    Chernenko, Volodymyr A.; Barandiarán, Jose M.; Rodriguez Fernández, Jesus; Rojas, Daniel P.; Gutiérrez, Jon; Lázpita, Patricia; Orue, Iñaki

    2012-01-01

    The evolutions of magnetic properties at low temperatures and the influence of magnetic field on the temperature dependence of specific heat in martensitic Ni 2 Mn 1.4 Sn 0.6 Heusler alloy are studied. The frequency-dependent blocking temperature and considerable exchange bias below it are measured in the martensitic phase. From the analysis of the specific heat curves under magnetic field, a large inverse magnetocaloric effect manifested as the magnetic field induced rise of isothermal magnetic entropy and/or magnetic field induced adiabatic temperature decrease in the vicinity of the reverse magnetostructural transformation and a significant value of the conventional magnetocaloric effect at the Curie temperature are obtained. The Debye temperature and electronic coefficient equal to Θ D =310±2 K and γ= 16.6±0.3 mJ/K 2 mol, respectively, do not depend on the magnetic field.

  13. Order-disorder structural phase transition and magnetocaloric effect in organic-inorganic halide hybrid (C2H5NH3)2CoCl4

    Science.gov (United States)

    Sen, Abhijit; Roy, Soumyabrata; Peter, Sebastian C.; Paul, Arpita; Waghmare, Umesh V.; Sundaresan, A.

    2018-02-01

    We report a detailed experimental and theoretical investigation of structural, optical, magnetic and magnetothermal properties of single crystals of a new organic-inorganic hybrid (C2H5NH3)2CoCl4. Grown by slow evaporation method at room temperature, the compound crystallizes in centrosymmetric orthorhombic structure (Pnma) which undergoes a reversible phase transition at 235/241 K (cooling/heating) to noncentrosymmetric P212121 space group symmetry associated with order-disorder transformation of carbon atoms of the ammonium cations as well as molecular rearrangement. Electronic absorption spectra of the compound are typical of geometrically distorted [CoCl4]2- tetrahedra having spin-orbit coupling effect. The isolated nature of [CoCl4]2- tetrahedra in the crystal reflect in paramagnetic behaviour of the compound. Interestingly, field induced spin flipping behaviour is observed at low temperature. First principles density functional calculations reveal weak magnetic interaction among cobalt spins with ferromagnetic state being the ground state. The entropy change associated with the spin flipping has been experimentally estimated by magnetic and heat capacity measurements which has a maximum value of 16 J Kg-1 K-1 at 2.5 K under 7 T magnetic field. To the best of our knowledge, this is the first report on magnetocaloric effect observed in an organic-inorganic halide compound. The estimated value is sizable and is comparable to that of well-known transition metal molecular cluster magnets Mn12 or Fe14. The overall findings promise to enlighten new routes to design and constitute multifunctional organic-inorganic halide materials.

  14. Magnetic and structural properties of high relative cooling power (Fe70Ni30)92Mn8 magnetocaloric nanoparticles

    Science.gov (United States)

    Chaudhary, V.; Ramanujan, R. V.

    2015-08-01

    Earth-abundant, low-cost, and rare earth free magnetocaloric nanomaterials have attracted considerable attention for affordable, ‘green’, energy-efficient thermal management applications. Hence, we investigated the magnetocaloric properties and critical behavior of (Fe70Ni30)92Mn8 alloy nanoparticles. A near room temperature magnetocaloric effect, with a high relative cooling power (RCP), was obtained by alloying FeNi with Mn and fcc (γ) phase stabilization. The Curie temperature (T C) of the γ- phase was 40 K less than that of the T C of the bcc (α) phase. For a field change of 5 T, the RCP for the α- and γ- phase was found to be 507 J kg-1 and 466 J kg-1, respectively; these values are higher than those for Gd nanoparticles. The RCP exhibited a power law relationship with magnetic field H. Critical exponents values of δ = 4.71, β = 0.319 and γ = 1.195 were obtained, close to those obtained from the short range order 3D-Heisenberg model. Our results demonstrate the feasibility of developing high RCP, low-cost, rare earth free magnetocaloric nanoparticles for near room temperature applications.

  15. Magnetocaloric effect and corrosion resistance of La(Fe, Si)13 composite plates bonded by different fraction of phenolic resin

    Science.gov (United States)

    Zhang, K. S.; Xue, J. N.; Wang, Y. X.; Sun, H.; Long, Y.

    2018-04-01

    La(Fe, Si)13-based composite plates were successfully fabricated using different amount of phenolic resin. The introduction of phenolic resin as binder increased the corrosion resistance and maintained giant magnetocaloric effect for La(Fe, Si)13-based composite plates. It was found that corroded spots were firstly observed on the boundaries between resin and La(Fe, Si)13 particles, rather than in La(Fe, Si)13-based particles, after being immersed in static distilled water. The corrosion rate decreased significantly with the increase of resin content. And the increase of the content of phenolic resin leads to the reduction of corrosion current density. Meanwhile, the volumetric magnetic entropy change ΔSM decreases slightly as the content of phenolic resin increases. The ΔSM of the plates with 3 wt.%, 5 wt.% and 8 wt.% resin are 63.1, 61.2 and 59.8 mJ/cm3 K under a low magnetic field change of 1 T, respectively.

  16. Toward a better understanding of the magnetocaloric effect: An experimental and theoretical study of MnFe4Si3

    Science.gov (United States)

    Gourdon, Olivier; Gottschlich, Michael; Persson, Joerg; Cruz, Clarina de la; Petricek, Vaclav; McGuire, Michael A.; Brückel, Thomas

    2014-08-01

    The intermetallic compound MnFe4Si3 has been studied by high-resolution Time of Flight (TOF) neutron powder diffraction. MnFe4Si3 crystallizes in the hexagonal space group P63/mcm with lattice constants of a=b=6.8043(4) Å and c=4.7254(2) Å at 310 K. Magnetic susceptibility measurements show clearly the magnetic transition from paramagnetism to ferromagnetism at about 302(2) K. Magnetic structure refinements based on neutron powder diffraction data with and without external magnetic field reveal strong evidence on the origin of the large magnetocaloric effect (MCE) in this material as a partial reordering of the spins between ~270 K and 300 K. In addition, electronic structure calculations using the self-consistent, spin-polarized Tight Binding-Linear MuffinTin Orbital (TB-LMTO) method were also accomplished to address the "coloring problem" (Mn/Fe site preference) as well as the unique ferromagnetic behavior of this intermetallic compound.

  17. Magnetocaloric properties of La0.666Sr0.373Mn0.943Cu0.018O3

    Directory of Open Access Journals (Sweden)

    Mahmoud A. Hamad

    2017-09-01

    Full Text Available Magnetocaloric properties of La0.666Sr0.373Mn0.943Cu0.018O3 (LSMCO perovskite (such as magnetic entropy change, full-width at half-maximum, relative cooling power and magnetic specific heat change at applied magnetic field of 0.05 T were calculated using the phenomenological model. The results indicate the prospective application of LSMCO due to high magnetocaloric effect near the Curie temperature. Furthermore, the magnetocaloric properties of LSMCO sample are comparable with magnetocaloric properties of MnAs film, La1-xCdxMnO3 and La1.25Sr0.75MnCoO6, and significantly larger than that of Gd1-xCaxBaCo2O5.5 and Ge0.95Mn0.05. It is recommended that magnetocaloric effect of LSMCO can be used as a promising practical material of an apparatus based on the active magnetic regenerator cycle.

  18. Effect of Fe substitution on the structure and magnetocaloric effect of Mn{sub 5−x}Fe{sub x}GeSi{sub 2} alloys

    Energy Technology Data Exchange (ETDEWEB)

    Sun, Y.W.; Yan, J.L., E-mail: yjl@gxu.edu.cn; Feng, E.L.; Tang, G.W.; Zhou, K.W.

    2017-01-15

    The structure and magnetocaloric effect of Mn{sub 5−x}Fe{sub x}GeSi{sub 2} compounds were studied. Analysis of X-ray powder diffraction and energy dispersive X-Ray spectroscopy revealed that Mn{sub 5−x}Fe{sub x}GeSi{sub 2} alloys with x<1 crystallize in the Mn{sub 5}Si{sub 3}-type structure (space group P6{sub 3}/mcm), maintaining the structure of Mn{sub 5}Ge{sub 3}; and alloys with x=1.5 and 2 consist of the major Mn{sub 5}Si{sub 3}-type phase and the minor Ni{sub 2}In-type phase (space group P6{sub 3}/mmc). The results of Rietveld refinement showed that the cell parameters for the Mn{sub 5}Si{sub 3}-type phase decrease with increasing Fe content. The positive slopes in Arrott plots indicate that a second-order ferromagnetic to paramagnetic transition occurs. The Curie temperature increases with increasing Fe content from 182 K for x=0.6 to 224 K for x=2. The maximum magnetic entropy change of 3.7 J/(kg K) for x=0.8 was found under a magnetic field change of 0–20 kOe. - Highlights: • Mn{sub 5−x}Fe{sub x}GeSi{sub 2} alloys with x<1 crystallize in the hexagonal Mn{sub 5}Si{sub 3}-type structure. Alloys with x=1.5 and 2 consist of a major Mn{sub 5}Si{sub 3}-type phase and a secondary Ni{sub 2}In-type phase. • The cell parameters decrease and the Curie temperature increases with increasing x in Mn{sub 5−x}Fe{sub x}GeSi{sub 2} alloys. • The maximum -∆S{sub M} of 3.7 J/(kg K) and RCP of 211 J/kg for x=0.8 was found under a magnetic field change of 0–20 kOe.

  19. Integration of a magnetocaloric heat pump in a low-energy residential building

    DEFF Research Database (Denmark)

    Johra, Hicham

    2018-01-01

    The EnovHeat project aims at developing an innovative heat pump system based on the magnetocaloric effect and active magnetic regenerator technology to provide for the heating needs of a single family house in Denmark. Unlike vapor-compression devices, magnetocaloric heat pumps use the reversible...... magnetocaloric effect of a solid refrigerant to build a cooling/heating cycle. It has the potential for high coefficient of performance, more silent operation and efficient part-load control. After presenting the operation principles of the magnetocaloric device and the different models used in the current...

  20. Pressure effects in the giant magnetocaloric compounds Gd5(SixGe1-x)4

    International Nuclear Information System (INIS)

    Morellon, L; Arnold, Z; Algarabel, P A; Magen, C; Ibarra, M R; Skorokhod, Y

    2004-01-01

    We report a study of the effect of hydrostatic pressure up to 9 kbar on selected compounds of the Gd 5 (Si x Ge 1-x ) 4 series (x = 0.8, 0.45, 0.1) by means of ac magnetic susceptibility, compressibility, and linear thermal expansion measurements. The pressure-induced increase of the transition temperatures at the second-order boundaries of the phase diagram is rather moderate: dT C /dP ∼ +0.3Kk-bar -1 (x = 0.8) and dT N /P ∼+0.7Kkbar -1 (x = 0.1). This effect is stronger in the 0 C /dP ∼ +3 Kk-bar -1 (x = 0.45,0.1), indicating that the ferromagnetic ordering can be simultaneously driven through a pressure-induced structural transformation. The values of d lnT C /d lnV calculated with the use of the measured value of compressibility (k ∼1.8 M-bar -1 ) are significantly lower than those estimated from the concentration dependence of the lattice cell volume, thus demonstrating that the dependence of the transition temperatures upon changing the Si/Ge ratio across the series cannot be explained by a pure volume effect

  1. The Effect of Magnetic Domains on the Measurement of the Magnetocaloric effect

    DEFF Research Database (Denmark)

    Bahl, Christian R.H.; Smith, Anders; Nielsen, Kaspar Kirstein

    2014-01-01

    We discuss how magnetic domains influence the magnetic entropy change calculated from magnetisation data. In a simple qualitative model we show that the effect is to change the shape of the apparent isothermal entropy change curve compared to the true curve determined by the entropy. We further s...

  2. Martensitic transition, inverse magnetocaloric effect and shape memory characteristics in Mn{sub 48−x}Cu{sub x}Ni{sub 42}Sn{sub 10} Heusler alloys

    Energy Technology Data Exchange (ETDEWEB)

    Liu, Changqin [Department of Physics, Shanghai University, Shanghai 200444 (China); Li, Zhe [Reasearch center for magnetic materials and devices & Key Laboratory for Advanced Functional and Low Dimensional Materials of Yunnan Higher Education Institute, Qujing Normal University, Qujing 655011 (China); Zhang, Yuanlei [Department of Physics, Shanghai University, Shanghai 200444 (China); Reasearch center for magnetic materials and devices & Key Laboratory for Advanced Functional and Low Dimensional Materials of Yunnan Higher Education Institute, Qujing Normal University, Qujing 655011 (China); Liu, Yang; Sun, Junkun; Huang, Yinsheng; Kang, Baojuan [Department of Physics, Shanghai University, Shanghai 200444 (China); Xu, Kun [Reasearch center for magnetic materials and devices & Key Laboratory for Advanced Functional and Low Dimensional Materials of Yunnan Higher Education Institute, Qujing Normal University, Qujing 655011 (China); Deng, Dongmei [Department of Physics, Shanghai University, Shanghai 200444 (China); Jing, Chao, E-mail: cjing@staff.shu.edu.cn [Department of Physics, Shanghai University, Shanghai 200444 (China)

    2017-03-01

    In this paper, we have systematically prepared a serials of polycrystalline Mn{sub 48−x}Cu{sub x}Ni{sub 42}Sn{sub 10} alloys (x=0, 1, 3, 5, 6, 8, 10 and 12) and investigated the influence of the Cu doping on martensitic transition (MT) as well as magnetic properties. Experimental results indicate that the MT temperature and the martensite Curie temperature (T{sub c}{sup M}) shift to high temperature with increasing the substitution of Cu (from Mn rich alloy to Ni rich alloy), while the austenite Curie temperature (T{sub c}{sup A}) is almost unchanged. It was found that the structures undergo L2{sub 1} and 4O with the increasing of Cu concentration near room temperature. Therefore, the magnetostructural transition can be tuned by appropriate Cu doping in these alloys. Moreover, we mainly studied the multiple functional properties for inverse magnetocaloric effect and shape memory characteristics associated with the martensitic transition. A large positive isothermal entropy change of Mn{sub 48}Ni{sub 42}Sn{sub 10} was obtained, and the maximum transition entropy change achieves about 48 J/kg K as x=8. In addition, a considerable temperature-induced spontaneous strain with the value of 0.16% was obtained for Mn{sub 48}Ni{sub 42}Sn{sub 10} alloys.

  3. Magnetocaloric and magnetoelastic effects in(Tb.sub.0.45./sub.Dy.sub.0.55./sub.).sub.1-x./sub.Er.sub.x./sub.Co.sub.2./sub. multicomponent compounds

    Czech Academy of Sciences Publication Activity Database

    Tereshina, I.; Politova, G.; Tereshina, Evgeniya; Nikitin, S.; Burkhanov, G.; Chistyakov, O.; Karpenkov, A.

    2010-01-01

    Roč. 200, č. 9 (2010), "092012-1"-"092012-4" ISSN 1742-6588. [International Conference on Magnetism - ICM 2009. Karlsruhe, 26.07.2009-31.07.2009] Institutional research plan: CEZ:AV0Z10100520 Keywords : terfenol-D * rare-earth Intermetallics * magnetostriction * magnetocaloric effect Subject RIV: BM - Solid Matter Physics ; Magnetism

  4. Magnetic field dependence of Griffith phase and magnetocaloric effect in Ca0.85Dy0.15MnO3

    Science.gov (United States)

    Nag, Ripan; Sarkar, Bidyut; Pal, Sudipta

    2018-03-01

    Temperature and Magnetic field dependent magnetization properties of electron doped polycrystalline sample Ca0.85Dy0.15MnO3 (CDMO) prepared by solid state reaction method have been studied. The sample undergoes ferromagnetic to paramagnetic phase transition at about 111k. From the study of magnetic properties in terms of Arrot plots it is observed that the phase transition is of 2nd order. The Griffith phase behavior of the sample is suppressed with the increase of the applied magnetic field strength H. We have estimated the magnetic entropy change from experimental magnetization and temperature data. For a magnetic field change of 8000 Oe, the maximum value of magnetic entropy change arrives at a value of 1.126 J-kg-1 k-1 in this magnetocaloric material.

  5. Some Aspects of Scaling and Universality in Magnetocaloric Materials

    DEFF Research Database (Denmark)

    Smith, Anders; Nielsen, Kaspar Kirstein; Bahl, Christian R.H.

    2014-01-01

    The magnetocaloric effect of a magnetic material is characterized by two quantities, the isothermal entropy change and the adiabatic temperature change, both of which are functions of temperature and applied magnetic field. We discuss the scaling properties of these quantities close to a second...... order phase transition within the context of critical scaling theory. In the critical region the isothermal entropy change will exhibit universal scaling exponents. However, this is only true close to Tc and for small fields; we show that for finite fields the scaling exponents in general become field...... dependent, even at Tc. Furthermore, the scaling exponents at finite fields are not universal: Two models with the same critical exponents can exhibit markedly different scaling behaviour even at relatively low fields. Turning to the adiabatic temperature change, we argue that it is not determined...

  6. Enhanced magnetocaloric effect tuning efficiency in Ni-Mn-Sn alloy ribbons

    Science.gov (United States)

    Quintana-Nedelcos, A.; Sánchez Llamazares, J. L.; Daniel-Perez, G.

    2017-11-01

    The present work was undertaken to investigate the effect of microstructure on the magnetic entropy change of Ni50Mn37Sn13 ribbon alloys. Unchanged sample composition and cell parameter of austenite allowed us to study strictly the correlation between the average grain size and the total magnetic field induced entropy change (ΔST). We found that a size-dependent martensitic transformation tuning results in a wide temperature range tailoring (>40 K) of the magnetic entropy change with a reasonably small variation on the peak value of the total field induced entropy change. The peak values varied from 6.0 J kg-1 K-1 to 7.7 J kg-1 K-1 for applied fields up to 2 T. Different tuning efficiencies obtained by diverse MCE tailoring approaches are compared to highlight the advantages of the herein proposed mechanism.

  7. Enhancement of Magnetocaloric Effect in ({ {La}}_{0.67}{ {Ca}}_{0.33}{ {MnO}}_{3})/({ {La}}_{0.7}{ {Ba}}_{0.3}{ {MnO}}_{3}) ( La 0.67 Ca 0.33 MnO 3 ) / ( La 0.7 Ba 0.3 MnO 3 ) Composite

    Science.gov (United States)

    Khelifi, J.; Dhahri, E.; Hlil, E. K.

    2018-03-01

    The composite (La_{0.67}Ca_{0.33}MnO3)/La_{0.7}Ba_{0.3}MnO3) sample was prepared using the conventional solid-state reaction method, and their crystallographic structure was achieved by X-ray diffraction pattern analysis. The magnetic and magnetocaloric effect has been studied by magnetization measurements. Based on the relation: χ ^{-1}(T)∝ (T-T_C^Rand )^{1-λ }, the inverse of susceptibility shows a downturn before T_C indicating the existence of Griffiths phase for the temperature range T_C^Randphase has been obtained from detailed magnetization studies. Furthermore, a large magnetic entropy change is observed in (La_{0.67}Ca_{0.33}MnO3)/(La_{0.7}Ba_{0.3}MnO3) composite which possesses a large MCE characterized by two Δ S_M(T) peaks. It has revealed that the combination of manganite materials with different Curie temperatures is a possible method for enhancement of magnetocaloric effect. To determine the field dependence of the experimental Δ S_M(T), a local exponent n( T, H) can be calculated from the logarithmic derivative of the magnetic entropy change versus field; it is shown that for a multiphase system n evolves with field both at the Curie temperature of the system and at the Curie temperatures of the constituent phases.

  8. Magnetocaloric features of complex molecular magnets: The (Cr7Ni)2Cu molecular magnet and beyond

    International Nuclear Information System (INIS)

    Florez, J.M.; Nunez, Alvaro S.; Garcia, C.; Vargas, P.

    2010-01-01

    We study the new kind of systems represented by the Cr 7 Ni-M-Cr 7 Ni (M=Cu +2 ) molecule, which is a promising molecular achievement from the perspective of molecular electronics. By using an effective quantum Hamiltonian, an exact calculation of the magnetic specific heat C Mag and the magnetocaloric features, namely, the adiabatic change of the entropy ΔS Mag and temperature ΔT ad , respectively, are developed. A systematic simulation of the magnetocaloric properties is generated by modifying the effective exchange couplings into the molecular system. Extended discussion of calculated magnetocaloric features and its possible realization by experimental methods, are performed. In addition, comparisons with an exact numerical result and with a Van Vleck transformation, which has important application in similar micromagnetic structures with no exact analytical solution and larger Hilbert space, are presented. Moreover, an expression for the entangling-excitation frequencies of these systems is given as first application of our simplified solution to the effective molecular Hamiltonian.

  9. Impacts of nanostructuring and magnetic ordering of Nd{sup 3+} on the magnetic and magnetocaloric response in NdMnO{sub 3}

    Energy Technology Data Exchange (ETDEWEB)

    Chandra, Sayan, E-mail: schandr5@mail.usf.edu; Biswas, Anis, E-mail: biswas.anis@gmail.com; Phan, Manh-Huong, E-mail: phanm@usf.edu; Srikanth, Hariharan, E-mail: sharihar@usf.edu

    2015-06-15

    Magnetocaloric properties of NdMnO{sub 3} were investigated in its bulk polycrystalline and nanocrystalline forms. The nanocrystalline sample (average particle size ∼40 nm) exhibits a maximum in the temperature dependence of magnetic entropy change [−ΔS{sub M}(T)] at ∼70 K due to the paramagnetic to ferromagnetic transition, which is absent in case of its bulk counterpart. The absence of peak in −ΔS{sub M}(T) in the bulk sample is attributed to the co-existence of antiferromagnetic and ferromagnetic phases. A canted magnetic state (CMS) is stabilized at low temperature for both the samples due to the ordering of Nd{sup 3+} giving rise to a peak in −ΔS{sub M}(T) at ∼15 K. Interestingly −ΔS{sub M}(T) for these two samples show a universal behavior near their transitions at low temperature although their temperature dependence of magnetization is markedly different around those transitions. A detailed analysis of magnetocaloric data conclusively establishes the existence of a canted magnetic state, which is not obvious from magnetometry, demonstrating the usefulness of this method for probing phase coexistence and multiple magnetic states in complex oxide systems. - Highlights: • Effect of reduction of particle size on magnetocaloric properties of NdMnO{sub 3} has been investigated. • The roles of Nd{sup 3+}-ordering and self-doping effect on magnetic and magnetocaloric properties of NdMnO{sub 3} have been discussed. • Nanocrystalline NdMnO{sub 3} exhibits large magnetocaloric effect (MCE) in two temperature regimes in contrary to bulk sample. • We emphasize how MCE study can be exploited to explore fundamental physics of magnetism.

  10. Materials Challenges for High Performance Magnetocaloric Refrigeration Devices

    DEFF Research Database (Denmark)

    Smith, Anders; Bahl, Christian; Bjørk, Rasmus

    2012-01-01

    Magnetocaloric materials with a Curie temperature near room temperature have attracted signifi cant interest for some time due to their possible application for high-effi ciency refrigeration devices. This review focuses on a number of key issues of relevance for the characterization, performance...

  11. Magnetic properties and magnetocaloric effect in the HoNi{sub 1−x}Cu{sub x}In (x=0, 0.1, 0.3, 0.4) intermetallic compounds

    Energy Technology Data Exchange (ETDEWEB)

    Mo, Zhao-Jun [School of Material Science and Engineering, Hebei University of Technology, Tianjin (China); Key Laboratory of Cryogenics, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing (China); Shen, Jun, E-mail: jshen@mail.ipc.ac.cn [Key Laboratory of Cryogenics, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing (China); Yan, Li-Qin [State Key Laboratory of Magnetism, Beijing National Laboratory for Condensed Matter, Physics and Institute of Physics, Chinese Academy of Sciences, Beijing (China); Tang, Cheng-Chun [School of Material Science and Engineering, Hebei University of Technology, Tianjin (China); He, Xiao-Nan [Key Laboratory of Cryogenics, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing (China); Zheng, Xinqi [State Key Laboratory of Magnetism, Beijing National Laboratory for Condensed Matter, Physics and Institute of Physics, Chinese Academy of Sciences, Beijing (China); Wu, Jian-Feng [Key Laboratory of Cryogenics, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing (China); Sun, Ji-Rong; Shen, Bao-Gen [State Key Laboratory of Magnetism, Beijing National Laboratory for Condensed Matter, Physics and Institute of Physics, Chinese Academy of Sciences, Beijing (China)

    2014-03-15

    The magnetic properties and magnetocaloric effect (MCE) in HoNi{sub 1−x}Cu{sub x}In (x=0, 0.1, 0.3, 0.4) compounds have been investigated. With the substitution of Cu for Ni, the Ho magnetic moment will cant from the c-axis, and form a complicated magnetic structure. These compounds exhibit two successive magnetic transitions with the increase in temperature. The large reversible magnetocaloric effects have been observed in HoNi{sub 1−x}Cu{sub x}In compounds around T{sub ord}, with no thermal and magnetic hysteresis loss. The large reversible isothermal magnetic entropy change (−ΔS{sub M}) is 20.2 J/kg K and the refrigeration capacity (RC) reaches 356.7 J/kg for field changes of 5 T for HoNi{sub 0.7}Cu{sub 0.3}In. Especially, the value of −ΔS{sub M} (12.5 J/kg K) and the large RC (132 J/kg) are observed for field changes of 2 T for HoNi{sub 0.9}Cu{sub 0.1}In. Additionally, the values of RC are improved to 149 J/K for the field changes of 2 T due to a wide temperature span for the mix of HoNi{sub 0.9}Cu{sub 0.1}In and HoNi{sub 0.7}Cu{sub 0.3}In compounds with the mass ratio of 1:1. These compounds with excellent MCE are expected to have effective applications in magnetic refrigeration around 20 K. - Highlights: • For magnetic-field changes of 2 T, the values of RC are improved to 149 J/K. • MCEs of these compounds show no thermal and magnetic hysteresis. • Compounds show two successive magnetic transitions with the increase in temperature. • With the substitution of Cu for Ni, compounds form a complicated magnetic structure.

  12. Enhanced magneto-caloric effect upon Co substitution in Ni-Mn-Sn thin films

    Science.gov (United States)

    Modak, Rajkumar; Raja, M. Manivel; Srinivasan, A.

    2018-02-01

    Mn rich Ni-Mn-Sn and Ni-Mn-Co-Sn alloy films were deposited on Si (1 0 0) substrate by dc magnetron sputtering from Ni50Mn37Sn13 alloy target at 1.8 Pa Ar pressure with 70 W dc power. Co was introduced by placing Co chips on the Ni-Mn-Sn target. As-deposited films were vacuum annealed at 823 K for 1 h. X-ray diffraction patterns of the films revealed modulated 14 M structure of the martensite phase at room temperature. Magnetic entropy change (ΔSm) across the Curie temperature of the ferromagnetic films was estimated from initial isothermal magnetization curves using Maxwell's equation. ΔSm and refrigeration capacity (RC) of Ni-Mn-Sn and Ni-Mn-Co-Sn films increased with increasing film thickness. Upon Co substitution in Mn/Sn site(s), ΔSm and RC increased more remarkably. The change is more prominent in the case of 360 nm films, wherein a 3.8-fold increase in ΔSM and 8.9-fold increase in RC was observed. Introduction of Co increased the magnetic moment and broadened the magnetic transition. These factors increased ΔSm and RC in Co substituted Ni-Mn-Sn alloy. Since TC shifted to higher temperatures with Co substitution, operating temperature of these magnetic refrigerants also shifted to higher temperature. This study indicates the possibility of developing high temperature cooling devices and waste energy harvesters using these films.

  13. Iron-based composition for magnetocaloric effect (MCE) applications and method of making a single crystal

    Science.gov (United States)

    Evans, III, Boyd Mccutchen; Kisner, Roger A.; Ludtka, Gail Mackiewicz; Ludtka, Gerard Michael; Melin, Alexander M.; Nicholson, Donald M.; Parish; , Chad M.; Rios, Orlando; Sefat, Athena S.; West, David L.; Wilgen, John B.

    2016-02-09

    A method of making a single crystal comprises heating a material comprising magnetic anisotropy to a temperature T sufficient to form a melt of the material. A magnetic field of at least about 1 Tesla is applied to the melt at the temperature T, where a magnetic free energy difference .DELTA.G.sub.m between different crystallographic axes is greater than a thermal energy kT. While applying the magnetic field, the melt is cooled at a rate of about 30.degree. C./min or higher, and the melt solidifies to form a single crystal of the material.

  14. Magnetocaloric heat pump device, a heating or cooling system and a magnetocaloric heat pump assembly

    DEFF Research Database (Denmark)

    2014-01-01

    The invention provides a magnetocaloric heat pump device, comprising a magnetocaloric bed; a magnetic field source, the magnetocaloric bed and the magnetic field source being arranged to move relative to each other so as to generate a magnetocaloric refrigeration cycle within the heat pump, wherein...

  15. Influence of magnetic frustration and structural disorder on magnetocaloric effect and magneto-transport properties in La1.5Ca0.5CoMnO6 double perovskite

    Science.gov (United States)

    Sahoo, R. C.; Das, Sananda; Nath, T. K.

    2018-01-01

    The rare existence of a magnetocaloric effect, a Griffith phase, and frustrated magnetism in the antisite disorder compound La1.5Ca0.5CoMnO6 have been investigated in detail in this work. The nature of the observed Griffith phase (at TG ˜ 226 K) can be best understood in terms of ferromagnetic (FM) entities within the globally paramagnetic network above the Curie temperature. From the isothermal magnetization measurement around Curie temperature (TC ˜ 157 K) and cluster glass transition temperature (Tg ˜ 51 K), we have determined the maximum entropy change (-ΔSM) as ˜2.2 J/kg K and ˜1.2 J/kg K, respectively, for a magnetic field variation of 7 T. Interestingly, a sudden drop of resistivity curve at Tg, associated with magnetic frustration or magnetic disorder, can be related to the ferromagnetic (FM) phases with antiferromagnetic antiphase boundaries, giving rise to a large negative magnetoresistance (˜67%) at 45 K.

  16. Large magnetocaloric effect in lanthanum-deficiency manganites La{sub 0.8−x}□{sub x}Ca{sub 0.2}MnO{sub 3} (0.00≤x≤0.20) with a first-order magnetic phase transition

    Energy Technology Data Exchange (ETDEWEB)

    Skini, R.; Omri, A. [Laboratoire de Physique Appliquée, Faculté des Sciences de Sfax, Université de Sfax, B.P. 802, Sfax 3018 (Tunisia); Khlifi, M., E-mail: khlifimouadh3000@yahoo.fr [Laboratoire de Physique Appliquée, Faculté des Sciences de Sfax, Université de Sfax, B.P. 802, Sfax 3018 (Tunisia); Dhahri, E. [Laboratoire de Physique Appliquée, Faculté des Sciences de Sfax, Université de Sfax, B.P. 802, Sfax 3018 (Tunisia); Hlil, E.K. [Institut Néel, CNRS et Université Joseph Fourier, BP 166, F-38042, Grenoble cedex 9 (France)

    2014-09-01

    Lanthanum-deficiency effect on the magnetic and magnetocaloric properties of La{sub 0.8−x}□{sub x}Ca{sub 0.2}MnO{sub 3} (0.00≤x≤0.20) polycrystalline samples has been investigated using X-ray diffraction and magnetization measurements. The structural characterization has revealed that all samples are crystallized in the orthorhombic structure with Pnma space group. From magnetic measurement a first-order magnetic phase transition from ferromagnetic to paramagnetic state is observed at the Curie temperature (T{sub C}) which is found to increase from 236.5 to 247 K when lanthanum-deficiency rate increases. Besides, both magnetocaloric effect (MCE) and relative cooling power (RCP) has been estimated. As important result, the values of MCE and RCP in our managanite with Lanthanum-deficiency are reported to be near to those found in the gadolinium considered as magnetocaloric material reference. Finally, the first-order magnetic phase transition has been confirmed by the construction of the universal curve of the magnetic entropy change. - Highlights: • La{sub 0.8−x}□{sub x}Ca{sub 0.2}MnO{sub 3} compounds crystallize in a Pnma orthorhombic symmetry. • All La{sub 0.8−x}□{sub x}Ca{sub 0.2}MnO{sub 3} compounds present large magnetic entropy change. • Our compounds can be considered as a good candidate for the magnetic refrigeration. • First-order phase transition is confirmed by the universal ΔS{sub M}(θ) curve.

  17. Magnetocaloric and magnetoresistive properties of La0.67Ca0.33-xSrxMnO3

    DEFF Research Database (Denmark)

    Dinesen, Anders Reves

    This thesis presents results of an experimental investigation of magneto-caloric and magnetoresistive properties of a series of polycrystalline Ca- and Sr-doped lanthanum manganites, La0.67Ca0.33-xSrxMnO3 (0=x=0.33 ), with the perovskite structure. The samples consisted of sintered oxide powders...... a magnetocaloric effect comparable to that of Gadolinium, the prototypical working material for magnetic refrigeration at room temperature. A less comprehensive part of the investigation regarded the magnetoresistive properties of the La0.67Ca0.33-xSrxMnO3 system. It was found that the polycrystalline nature...... of the compounds played a decisive role for the magnetotransport properties. Characteristic grain boundary effects, such as a low-field magnetoresistance, which is absent in single-crystalline perovskites, were observed. The low-field effect is usually ascribed to spin-dependent scattering in grain boundaries...

  18. Negative and positive magnetocaloric effect in Ni-Fe-Mn-Ga alloy

    International Nuclear Information System (INIS)

    Duan Jingfang; Huang Peng; Zhang Hu; Long Yi; Wu Guangheng; Rongchang Ye; Chang Yongqin; Farong Wan

    2007-01-01

    The phase transition process and magnetic entropy change ΔS of Ni 54.5 FeMn 20 Ga 24.5 alloy were studied. Substitution of Fe for Ni increases the Curie temperature and decreases the temperature of martensitic phase transition. The transition from ferromagnetic martensitic to ferrormagnetic austenitic state leads to an abrupt increase of magnetization below 0.5T and an abrupt decrease of magnetization above 0.5T. The sign of ΔS changes from positive to negative with increasing the applied field from 0.5 to 2T. The maximal value of the positive magnetic entropy change ΔS is about 3.1J/kgK for the applied field from 0 to 0.5T. The increase of applied field from 1.5T results in a negative ΔS. The peak of negative ΔS is -2.1J/kgK for a field change of 2T

  19. Magnetocaloric effect in multiferroic Y-type hexaferrite Ba0.5Sr1.5Zn2(Fe0.92Al0.0812O22

    Directory of Open Access Journals (Sweden)

    Wenfei Xu

    2014-06-01

    Full Text Available Magnetocaloric effect is investigated in multiferroic Ba0.5Sr1.5Zn2(Fe0.92Al0.0812O22 ceramic with Y-type hexagonal system. Three magnetic transitions, from alternating longitudinal conical to mixed conical at ∼240 K, to ferrimagnetic at ∼297 K, further to paramagnetic at ∼702 K, are unambiguously determined. Furthermore, obvious MCE is shown, and the maximum values of the magnetic entropy change and relative cooling power are evaluated to be 1.53 JKg−1K−1 and 280 JKg−1 for a field change of 7 T, respectively. In addition, inverse MCE is also observed, which might be associated with the first-order magnetic phase transition between two incommensurate longitudinal conical phases.

  20. Structural, magnetic and magnetocaloric properties of (Mn, Co){sub 2}(Si, P) compounds

    Energy Technology Data Exchange (ETDEWEB)

    Ma, Lei, E-mail: malei2010@163.com [Fundamental Aspects of Materials and Energy (FAME), Faculty of Applied Science, Delft University of Technology, Mekelweg 15, 2629 JB Delft (Netherlands); School of Materials Science and Engineering, Guilin University of Electronic Technology, Guilin 541004 (China); Guillou, F.; Yibole, H.; Miao, X.F.; Lefering, A.J.E. [Fundamental Aspects of Materials and Energy (FAME), Faculty of Applied Science, Delft University of Technology, Mekelweg 15, 2629 JB Delft (Netherlands); Rao, G.H.; Gu, Z.F.; Cheng, G. [School of Materials Science and Engineering, Guilin University of Electronic Technology, Guilin 541004 (China); Brück, E. [Fundamental Aspects of Materials and Energy (FAME), Faculty of Applied Science, Delft University of Technology, Mekelweg 15, 2629 JB Delft (Netherlands)

    2015-03-15

    Highlights: • Mn{sub 1.2}Co{sub 0.8}Si{sub 0.2}P{sub 0.8} shows an antiferro–ferromagnetic transition at 235 K. • Addition of B leads to an increase of the transition temperature T{sub N}. • A modest inverse magnetocaloric effect is observed at T{sub N}. - Abstract: We report on various approaches to control the antiferro–ferromagnetic transition temperature of Mn{sub 1.2}Co{sub 0.8}Si{sub 0.2}P{sub 0.8} and related materials for magnetocaloric applications. The effects of the Si substitution, Mn/Co ratio and B addition/substitution on MnCoP have been characterized by X-ray diffraction and magnetic measurements. In each case, these parameters have a great influence on the structural and magnetic properties. Silicon and boron turn out to be the elements suitable to substitute the phosphorous and bring T{sub N} closer to room temperature. The study thus paves the way for future tuning of the working temperature and adjustment of the magnetic properties. With entropy change of about 1.4 J kg{sup −1} K{sup −1} for 5 T, the inverse magnetocaloric effect of Mn{sub 1.2}Co{sub 0.8}Si{sub 0.2}P{sub 0.8} is modest, but might present some interest for applications other than magnetic cooling.

  1. Structural, magnetic and magnetocaloric properties of Heusler alloys Ni50Mn38Sb12 with boron addition

    DEFF Research Database (Denmark)

    Van Nong, Ngo; Tai, N.T.; Huy, N.T.

    2011-01-01

    We report on the structural, magnetic and magnetocaloric properties of the Ni50Mn38Sb12Bx alloys in term of boron addition with x=1, 3 and 5. We have found that both the paramagnetic–ferromagnetic austenitic transition (TC) and the ferromagnetic–antiferromagnetic martensitic transition (TM......) are sensitively influenced by the boron addition: TC tends to increase, while TM decreases with increasing boron concentration. Temperature dependent X-ray diffraction in the range of 200–500K clearly shows an evolution of the structural transformation from orthorhombic to cubic structure phase transition...... on heating for the x=1 and 3 samples. Strikingly, the addition of boron atoms into the lattice favours the ferromagnetic ordering relatively to the antiferromagnetic arrangement below TM. This consequently affects on the magneto-structural transition as well as on the size of magnetocaloric effect....

  2. Structural, magnetic and magnetocaloric properties of EuMnO3 perovskite manganite: A comprehensive MCE study

    Science.gov (United States)

    Phebe Kokila, I.; Kanagaraj, M.; Sathish Kumar, P.; Peter, Sebastian C.; Sekar, C.; Annal Therese, Helen

    2018-02-01

    Pervoskite manganite EuMnO3 synthesized by solid-state route was studied for their structural and magnetocaloric properties. EuMnO3 formed a single phase compound in orthorhombic crystal structure with a space group of Pbnm. The zero field cooling and field cooling magnetic responses exhibit an optimal Neel temperature (TN) of 57 K. A stronger magnetic coupling between the EuMnO3 particles are observed by a delay in reaching TN. The magnetocaloric effect analyzed extensively from the negative entropy (‑ΔSm) change of 15.23 JKg‑1K‑1 for EuMnO3, exhibited a Relative Cooling Power (RCP) of ∼211 JKg‑1 at 1.2 T proposing EuMnO3 as a potential magnetic refrigerant.

  3. Magnetocaloric as a sensitive tool to study magnetic phase in Ca4Mn3O10-δ

    Science.gov (United States)

    Mondal, Sampad; Modak, M.; Ray, M. K.; Mandal, Swapan K.; Sardar, M.; Banerjee, S.

    2018-02-01

    We report here magnetic properties of non-stoichiometric Ca4Mn3O10-δ . We have measured magnetization, electrical resistance, magnetoresistance, specific heat and thermo remanent magnetization (TRM) relaxation measurements. We find that at temperatures above 75 K the electrical transport can be explained in terms of activated hopping of magnetic polarons. These polarons are formed due to oxygen vacancy inducing Mn3+ sites. Below 50 K the polarons begins to strongly localize causing loss of moment and the electrical transport is governed by variable range hopping (VRH) conduction. The system shows glassy spin relaxation below 50 K, which presumably evolves into cluster spin glass at 12 K due to short range ordering of the canted moments. All these aspect could be well correlated with characteristics signature from magnetocaloric effect indicating magnetocaloric is a sensitive tool to study magnetic phase.

  4. Influence of Ti Doping on the Critical Behavior and Magnetocaloric Effect in Disordered Ferromagnets La0.7Ba0.3Mn1- x Ti x O3

    Science.gov (United States)

    Ho, T. A.; Phan, M. H.; Phuc, N. X.; Lam, V. D.; Phan, T. L.; Yu, S. C.

    2016-05-01

    The Ti-substitution influence on the magnetic and magnetocaloric properties of La0.7Ba0.3Mn1- x Ti x O3 ( x = 0.05 and 0.1) was investigated. Based on Banerjee's criteria and Franco's universal curves, we proved the existence of a second-order magnetic phase transition in the samples. Using the modified Arrott plot method, we determined the critical parameters T C ≈ 245 K, β = 0.374 ± 0.013, γ = 1.228 ± 0.045, and δ = 4.26 ± 0.03 for x = 0.05, and T C ≈ 169 K, β = 0.339 ± 0.001, γ = 1.307 ± 0.003, and δ = 4.78 ± 0.02 for x = 0.1. With these critical values, the predictable scaling behavior of the M( H) data above and below T C proves that the calculated exponents are unambiguous and intrinsic. The values β = 0.374 for x = 0.05 and β = 0.339 for x = 0.1 suggest that the magnetic phase transition of the samples falls into the three-dimensional (3D) Heisenberg and 3D Ising universality classes, respectively, corresponding to short-range ferromagnetic (FM) order due to FM clusters in a wide temperature range even above T C, as confirmed by electron spin resonance studies. In reference to the magnetocaloric effect around T C, the magnetic entropy change reaches maximum values (|ΔSmax|) of about 4 and 3 J kg-1 K-1 for x = 0.05 and 0.1, respectively, for a magnetic field change 50 kOe. Magnetic field dependencies of |ΔSmax| obey a power function |ΔSmax( H)| ∝ H n , where exponent values n = 0.59 and 0.61 for x = 0.05 and 0.1, respectively, were determined from the relation n = 1 + ( β-1)/( β + γ). The difference between the experimental n values and the theoretical value n = 2/3 of the mean field model is due to the presence of short-range FM order in the samples.

  5. The effect of cooling rate on the phase formation and magnetocaloric properties in La0.6Ce0.4Fe11.0Si2.0 alloys

    Science.gov (United States)

    Yang, Jian; Shao, Yanyan; Feng, Zaixin; Liu, Jian

    2018-04-01

    In this work, the microstructure, phase formation behavior of the NaZn13-type 1:13 phase and related magnetocaloric effect have been investigated in La0.6Ce0.4Fe11.0Si2.0 as-cast bulk and melt-spun ribbons with different cooling rates. A multi-phase structure consisting of 1:13, α-Fe and La-rich phases is observed in the induction-melted sample with slow cooling. By fast cooling in the melt spinning processing, the La-rich phase can be almost eliminated and thus 1:13 phases with volume fraction as high as 74.4% directly form in the absence of further heat treatment. The resulting maximum magnetic entropy change of 3.1 J/kg K in 2 T field appears at its Curie temperature of 210 K for the La0.6Ce0.4Fe11.0Si2.0 ribbon prepared in 25 m/s.

  6. Magnetic properties and magnetocaloric effect in the RCu{sub 2}Si{sub 2} and RCu{sub 2}Ge{sub 2} (R = Ho, Er) compounds

    Energy Technology Data Exchange (ETDEWEB)

    Mo, Zhao-Jun [School of Material Science and Engineering, Hebei University of Technology, Tianjin (China); Key laboratory of cryogenics, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing (China); Shen, Jun, E-mail: jshen@mail.ipc.ac.cn, E-mail: tangcc@hebut.edu.cn; Wu, Jian-Feng [Key laboratory of cryogenics, Technical Institute of Physics and Chemistry, Chinese Academy of Sciences, Beijing (China); Yan, Li-Qin; Wang, Li-Chen; Sun, Ji-rong; Shen, Bao-Gen [State Key Laboratory of Magnetism, Beijing National Laboratory for Condensed Matter, Physics and Institute of Physics, Chinese Academy of Sciences, Beijing (China); Gao, Xin-Qiang; Tang, Cheng-Chun, E-mail: jshen@mail.ipc.ac.cn, E-mail: tangcc@hebut.edu.cn [School of Material Science and Engineering, Hebei University of Technology, Tianjin (China)

    2014-02-21

    The magnetic properties and magnetocaloric effect (MCE) in RCu{sub 2}Si{sub 2} and RCu{sub 2}Ge{sub 2} (R = Ho, Er) compounds have been investigated. All these compounds possess an antiferromagnetic (AFM)-paramagnetic (PM) transition around their respective Neel temperatures. The RCu{sub 2}Si{sub 2} compounds undergo spin-glassy behavior above Neel temperature. Furthermore, a field-induced metamagnetic transition from AFM to ferromagnetic (FM) states is observed in these compounds. The calculated magnetic entropy changes show that all RCu{sub 2}Si{sub 2} and RCu{sub 2}Ge{sub 2} (R = Ho, Er) compounds, especially, ErCu{sub 2}Si{sub 2} exhibits large MCEs with no thermal hysteresis and magnetic hysteresis loss. The value of −ΔS{sub M}{sup max} reaches 22.8 J/Kg K for magnetic field changes from 0 to 5 T. In particular, for field changes of 1 and 2 T, the giant reversible magnetic entropy changes −ΔS{sub M}{sup max} are 8.3 and 15.8 J/kg K at 2.5 K, which is lower than the boiling point of helium. The low-field giant magnetic entropy change, together with ignorable thermal hysteresis and field hysteresis loss of ErCu{sub 2}Si{sub 2} compound is expected to have effective applications in low temperature magnetic refrigeration.

  7. Magnetostructural transformation and magnetocaloric effect in Mn48‑x V x Ni42Sn10 ferromagnetic shape memory alloys

    Science.gov (United States)

    Hassan, Najam ul; Shah, Ishfaq Ahmad; Khan, Tahira; Liu, Jun; Gong, Yuanyuan; Miao, Xuefei; Xu, Feng

    2018-03-01

    In this work, we tuned the magnetostructural transformation and the coupled magnetocaloric properties of Mn48‑x V x Ni42Sn10 (x = 0, 1, 2, and 3) ferromagnetic shape memory alloys prepared by means of partial replacement of Mn by V. It is observed that the martensitic transformation temperatures decrease with the increase of V content. The shift of the transition temperatures to lower temperatures driven by the applied field, the metamagnetic behavior, and the thermal hysteresis indicates the first-order nature for the magnetostructural transformation. The entropy changes with a magnetic field variation of 0–5 T are 15.2, 18.8, and 24.3 {{J}}\\cdot {kg}}-1\\cdot {{{K}}}-1 for the x = 0, 1, and 2 samples, respectively. The tunable martensitic transformation temperature, enhanced field driving capacity, and large entropy change suggest that Mn48‑x V x Ni42Sn10 alloys have a potential for applications in magnetic cooling refrigeration. Project supported by the National Natural Science Foundation of China (Grant Nos. 51601092, 51571121, and 11604148), the Fundamental Research Funds for the Central Universities, China (Grant Nos. 30916011344 and 30916011345), the Fund Program for the Scientific Activities of Selected Returned Overseas Professionals in Shanxi Province, China, the Postdoctoral Science Foundation Funded Project (Grant No. 2016M591851), the Natural Science Foundation of Jiangsu Province, China (Grant Nos. BK20160833, 20160829, and 20140035), the Qing Lan Project of Jiangsu Province, the Priority Academic Program Development of Jiangsu Higher Education Institutions, and Shanxi Scholarship Council of China (Grant No. 2016-092).

  8. Magnetocaloric piezoelectric composites for energy harvesting

    International Nuclear Information System (INIS)

    Cleveland, Michael; Liang, Hong

    2012-01-01

    Magnetocaloric alloy, Gd 5 Si 2 Ge 2 , was developed into a composite with the poly(vinylidene fluoride) (PVDF) piezoelectric polymer. This multifunctional material possesses unique properties that are suitable for energy conversion and harvesting. Experimental approaches include using an arc melting technique to synthesize the Gd 5 Si 2 Ge 2 (GSG) alloy and the spinning casting method to fabricate the composite. The materials were characterized using various techniques at different length scales. These include atomic force microscopy (AFM), optical microscopy, scanning electron microscopy (SEM) with energy dispersive spectroscopy (EDS), x-ray diffraction (XRD), and x-ray photoelectron spectroscopy (XPS). The results indicated that the phase transformation of the magnetocaloric material close to its Curie temperature induced a significant increase in power generation in the piezoelectric polymer. The power output of a laminated structure was 1.1 mW, more than 200 thousand times higher than the piezoelectric materials alone (5.1 nW). (technical note)

  9. Phase separation and magnetocaloric effect in Pr{sub 0.5−x}Gd{sub x} Sr{sub 0.5}MnO{sub 3} system

    Energy Technology Data Exchange (ETDEWEB)

    Bourouina, M. [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, Université de Sfax, B. P. 1171, 3000 Sfax (Tunisia); Krichene, A., E-mail: akramkri@hotmail.fr [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, Université de Sfax, B. P. 1171, 3000 Sfax (Tunisia); Chniba Boudjada, N. [Institut Néel, B.P. 166, 38042 Grenoble Cedex 9 (France); Boujelben, W. [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, Université de Sfax, B. P. 1171, 3000 Sfax (Tunisia)

    2016-09-25

    The magnetic properties and the magnetocaloric effect have been studied in Pr{sub 0.5−x}Gd{sub x}Sr{sub 0.5}MnO{sub 3} (x = 0, 0.05 and 0.1) manganites prepared by the solid state reaction method. Magnetic measurements versus temperature in an applied magnetic field of 0.05 T show that the all samples exhibit a paramagnetic to ferromagnetic transition when temperature decreases. The x = 0.1 sample shows a clear transition, from the ferromagnetic state to the antiferromagnetic one at T{sub N} = 125 K. The Curie temperature decreases gradually with increasing gadolinium content. The absolute values of the maximum of magnetic entropy change |ΔS{sub M}| for an applied magnetic field of 2 T are equal to1.26, 1.25 and 1.02 J kg{sup −1} K{sup −1} for x = 0, 0.05 and 0.1, respectively. The decrease of |ΔS{sub M}| with Gd doping can be attributed to the enhancement of phase separation phenomenon. The magnetic entropy curves follow the universal law corresponding to the second-ordered paramagnetic-ferromagnetic transition. - Highlights: • Gd doping in Pr{sub 0.5−x}Gd{sub x}Sr{sub 0.5}MnO{sub 3} (with x = 0, 0.05 and 0.1) enhances the antiferromagnetic interactions. • The studied samples are characterized by the phase separation phenomenon. • Magnetic properties are in agreement with electrical results.

  10. Integration of a magnetocaloric heat pump in a low-energy residential building

    DEFF Research Database (Denmark)

    Johra, Hicham; Filonenko, Konstantin; Heiselberg, Per

    2018-01-01

    magnetocaloric effect of a solid refrigerant to build a cooling/heating cycle. It has the potential for high coefficient of performance, more silent operation and efficient part-load control. After presenting the operation principles of the magnetocaloric device and the different models used in the current......The EnovHeat project aims at developing an innovative heat pump system based on the magnetocaloric effect and active magnetic regenerator technology to provide for the heating needs of a single family house in Denmark. Unlike vapor-compression devices, magnetocaloric heat pumps use the reversible...... heat pump can deliver 2600 W of heating power with an appreciable average seasonal system COP of 3.93. On variable part-load operation with a simple fluid flow controller, it can heat up an entire house with an average seasonal system COP of 1.84....

  11. Magnetocaloric effect and negative thermal expansion in hexagonal Fe doped MnNiGe compounds with a magnetoelastic AFM-FM-like transition.

    Science.gov (United States)

    Xu, Kun; Li, Zhe; Liu, Enke; Zhou, Haichun; Zhang, Yuanlei; Jing, Chao

    2017-01-30

    We report a detailed study of two successive first-order transitions, including a martensitic transition (MT) and an antiferromagnetic (AFM)-ferromagnetic (FM)-like transition, in Mn 1-x Fe x NiGe (x = 0, 0.06, 0.11) alloys by X-ray diffraction, differential scanning calorimetry, magnetization and linear thermal expansion measurements. Such an AFM-FM-like transition occurring in the martensitic state has seldom been observed in the M(T) curves. The results of Arrott plot and linear relationship of the critical temperature with M 2 provide explicit evidence of its first-order magnetoelastic nature. On the other hand, their performances as magnetocaloric and negative thermal expansion materials were characterized. The isothermal entropy change for a field change of 30 kOe reaches an impressive value of -25.8 J/kg K at 203 K for x = 0.11 compared to the other two samples. It demonstrates that the magneto-responsive ability has been significantly promoted since an appropriate amount of Fe doping can break the local Ni-6Mn AFM configuration. Moreover, the Fe-doped samples reveal both the giant negative thermal expansion and near-zero thermal expansion for different temperature ranges. For instance, the average thermal expansion coefficient ā of x = 0.06 reaches -60.7 × 10 -6 /K over T = 231-338 K and 0.6 × 10 -6 /K over T = 175-231 K during cooling.

  12. Magnetic and magnetocaloric properties of DyMn{sub 2}Si{sub 2} compound with multiple magnetic phase transition

    Energy Technology Data Exchange (ETDEWEB)

    Reis, D.C. dos; França, E.L.T. [Centro de Ciências Sociais Saúde e Tecnologia (CCSST), Universidade Federal do Maranhão – UFMA R. Urbano Santos, s/n, 65900-410 Imperatriz, Maranhão (Brazil); Paula, V.G. de [Instituto de Física “Gleb Wataghin”, Universidade Estadual de Campinas – UNICAMP, R. Sérgio Buarque de Holanda, 777, 13083-859 Campinas, São Paulo (Brazil); Santos, A.O. dos [Centro de Ciências Sociais Saúde e Tecnologia (CCSST), Universidade Federal do Maranhão – UFMA R. Urbano Santos, s/n, 65900-410 Imperatriz, Maranhão (Brazil); Coelho, A.A.; Cardoso, L.P. [Instituto de Física “Gleb Wataghin”, Universidade Estadual de Campinas – UNICAMP, R. Sérgio Buarque de Holanda, 777, 13083-859 Campinas, São Paulo (Brazil); Silva, L.M. da, E-mail: luzeli.moreira@ufma.br [Centro de Ciências Sociais Saúde e Tecnologia (CCSST), Universidade Federal do Maranhão – UFMA R. Urbano Santos, s/n, 65900-410 Imperatriz, Maranhão (Brazil)

    2017-02-15

    Structural, magnetic and magnetocaloric properties of the ternary intermetallic compound DyMn{sub 2}Si{sub 2} are studied by X-ray diffraction and magnetization measurements. It is found that DyMn{sub 2}Si{sub 2} crystalizes with tetragonal ThCr{sub 2}S{sub 2}-type structure and exhibits four successive magnetic transitions at low temperature, around 20 K, 31 K, 38 K and 82 K, named respectively as T{sub 1}, T{sub 2}, T{sub 3} and T{sub 4} transitions. Large values of magnetic field (>35 kOe) favor antiferromagnetic clusters and give rise to exchange bias effect. The different responses of T{sub 2} and T{sub 3} to field change, induces two non-identical isothermal entropy change (-ΔS{sub M}) peaks. The maximum values of -ΔS{sub M} occur in temperatures around T{sub 3} and reaches 8.2 J/kgK, for a magnetic field change of 50 kOe. Also, the presence of transitions T{sub 2} and T{sub 3} close to each other induces a table-like magnetocaloric effect (MCE) in a wide temperature range. Thus, the peculiar magnetic properties observed for DyMn{sub 2}Si{sub 2} compound are interesting for low temperature magnetic refrigeration. - Highlights: • The ternary intermetallic compound DyMn{sub 2}Si{sub 2} is proposed as magnetocaloric material. • Four magnetic phase transitions were identified for DyMn{sub 2}Si{sub 2} at low temperatures. • H >35 kOe favor antiferromagnetic clusters and give rise to exchange bias effect. • Two successive magnetic phase transitions induce a large table like EMC.

  13. Development of Power Electronics Based Test Platform for Characterization and Testing of Magnetocaloric Materials

    Directory of Open Access Journals (Sweden)

    Deepak Elamalayil Soman

    2015-01-01

    Full Text Available Magnetocaloric effects of various materials are getting more and more interesting for the future, as they can significantly contribute towards improving the efficiency of many energy intensive applications such as refrigeration, heating, and air conditioning. Accurate characterization of magnetocaloric effects, exhibited by various materials, is an important process for further studies and development of the suitable magnetocaloric heating and cooling solutions. The conventional test facilities have plenty of limitations, as they focus only on the thermodynamic side and use magnetic machines with moving bed of magnetocaloric material or magnet. In this work an entirely new approach for characterization of the magnetocaloric materials is presented, with the main focus on a flexible and efficient power electronic based excitation and a completely static test platform. It can generate a periodically varying magnetic field using superposition of an ac and a dc magnetic field. The scale down prototype uses a customized single phase H-bridge inverter with essential protections and an electromagnet load as actuator. The preliminary simulation and experimental results show good agreement and support the usage of the power electronic test platform for characterizing magnetocaloric materials.

  14. Magneto-caloric and magneto-resistive properties of La0.67Ca0.33-xSrxMnO3

    International Nuclear Information System (INIS)

    Reves Dinesen, Anders

    2004-08-01

    This thesis presents results of an experimental investigation of magneto-caloric and magneto-resistive properties of a series of polycrystalline Ca- and Sr-doped lanthanum manganites, La 0.67 Ca 0.33-x Sr x MnO 3 (0≤ x ≤ 0.33), with the perovskite structure. The samples consisted of sintered oxide powders prepared the glycine-nitrate combustion technique. The compounds were ferromagnetic and showed a Curie transition in the temperature range 267370 K (T C increased with increasing x). An analysis of the structural properties was carried out by means of x-ray diffraction and the Rietveld technique. The variation of the Ca/Sr ratio was found to cause a transition from orthorhombic to rhombohedral symmetry in the composition range 0.110 0.67 Ca 0.33-x Sr x MnO 3 samples was measured directly and indirectly (by means of magnetization measurements). All the samples showed a magnetocaloric effect in the vicinity of T C . A model for the mag-netocaloric effect based on Weiss mean field theory and classical theories for heat capacities was developed. The model provided reasonable predictions of the magneto-caloric properties of the samples. The compounds with low Sr content showed a magnetocaloric effect comparable to that of Gadolinium, the prototypical working material for magnetic refrigeration at room temperature. A less comprehensive part of the investigation regarded the magneto-resistive properties of the La 0.67 Ca 0.33-x Sr x MnO 3 system. It was found that th polycrystalline nature of the compounds played a decisive role for the magnetotransport properties. Characteristic grain boundary effects, such as a low-field magnetoresistance, which is absent in single-crystalline perovskites, were observed. The low-field effect is usually ascribed to spin-dependent scattering in grain boundaries. Qualitatively the results obtained for the La 0.67 Ca 0.33-x Sr x MnO 3 samples were consistent with this model. The resistivity contribution arising from the presence of

  15. Magnetic, transport and magnetocaloric properties in the Laves phase intermetallic Ho (Co1−xAlx)2 compounds

    International Nuclear Information System (INIS)

    Ivanova, T.I.; Nikitin, S.A.; Tskhadadze, G.A.; Koshkid’ko, Yu.S.; Suski, W.; Iwasieczko, W.; Badurski, D.

    2014-01-01

    Highlights: • The Al influence on magnetic properties of the Ho (Co 1-x Al x ) 2 compounds is analyzed. • The first-order magnetic transition appears in sample with Al concentrations x ≤ 0.06. • The MCE and Curie temperature TC demonstrate complex Al concentration dependences. • The magnetoresistance for sample with Al concentration x = 0.06 (58%) is maximum. • High magnetic fields changes the Curie temperature T c of the Ho (Co 1−x Al x ) 2 compounds. - Abstract: The magnetization, magnetoresistivity and magnetocaloric effect (MCE) of the Ho (Co 1−x Al x ) 2 Laves phase intermetallic compounds for x ⩽ 0.2 have been investigated. Complex measurements have been carried out in order to determine the influence of substitution in the Co sublattice by Al on the Co moment, type of the magnetic transition and related properties of these compounds. A comparative analysis of the magnetic, transport and magnetocaloric properties of Ho (Co 1−x Al x ) 2 alloys under various Al concentration is represented. Substitutions at the Co site by Al are found to result in the appearance of itinerant electron metamagnetism (IEM) at the small Al concentrations and in positive magnetovolume effect, leading to an initial increase in the ordering temperature; on the other hand the magnetic phase transition temperature as well as ΔT (MCE) do not depend in direct way on the Al concentration. The 16% increase of magnetocaloric effect for the alloy with x = 0.02 is detected in relation to maternal HoCo 2 . A giant value of magnetoresistivity (58%) is observed for the alloy with the same Al concentration

  16. Phase control studies in Gd5Si2Ge2 giant magnetocaloric compound

    International Nuclear Information System (INIS)

    Belo, J.H.; Pereira, A.M.; Ventura, J.; Oliveira, G.N.P.; Araújo, J.P.; Tavares, P.B.; Fernandes, L.; Algarabel, P.A.; Magen, C.; Morellon, L.

    2012-01-01

    Highlights: ► Study of time dependence of O(I) to M phase. ► Determination of the optimal annealing time. ► New method for phase amount estimation (O(I) and M). ► Effect of annealing on the MCE. ► Analysis of the nature of the magnetic transition through the Arrot plot representation. - Abstract: A systematic set of annealings on arc-melted synthesized Gd 5 Si 2 Ge 2 sample was performed. Through powder X-ray diffraction (XRD) and magnetometry measurements we monitored the effect of varying the annealing time with constant temperature (T = 1473 K) on the formation of the monoclinic (M) crystallographic phase fraction, which is the one responsible for the giant magnetocaloric effect (GMCE) in this compound. The conversion of the orthorhombic O(I) crystallographic phase into M was achieved, resulting in a significant increase of the M mass fraction. Such conversion led to a change in the magnetic transition nature, evolving from a second to a first order transition for the as-cast and annealed samples, respectively. An optimal annealing time range for the M phase conversion was identified to be within 80–120 min at T = 1473 K followed by a rapid quenching to liquid N 2 . Furthermore, an increase up to ∼50% of the magnetocaloric effect was obtained for the sample annealed during 120 min.

  17. The effects of small metal additions (Co, Cu, Ga, Mn, Al, Bi, Sn) on the magnetocaloric properties of the Gd5Ge2Si2 alloy

    Czech Academy of Sciences Publication Activity Database

    Shull, R. D.; Provenzano, V.; Shapiro, A. J.; Fu, A.; Lufaso, M. W.; Karapetrova, J.; Kletetschka, Günther; Mikula, V.

    2006-01-01

    Roč. 99, č. 8 (2006), s. 8-8 ISSN 0021-8979 Institutional research plan: CEZ:AV0Z30130516 Keywords : magnetocaloric * (Co, Cu, Ga, Mn, Al, Bi, Sn) additions * Cryogenic properties Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 2.316, year: 2006

  18. Structural flexibility in magnetocaloric RE5T4 (RE=rare-earth; T=Si,Ge,Ga) materials: Effect of chemical substitution on structure, bonding and properties

    Energy Technology Data Exchange (ETDEWEB)

    Misra, Sumohan [Iowa State Univ., Ames, IA (United States)

    2008-01-01

    The binary, ternary and multicomponent intermetallic compounds of rare-earth metals (RE) with group 14 elements (Tt) at the RE5Tt4 stoichiometry have been known for over 30 years, but only in the past decade have these materials become a gold mine for solid-state chemistry, materials science and condensed matter physics. It all started with the discovery of a giant magnetocaloric effect in Gd5Si2Ge2, along with other extraordinary magnetic properties, such as a colossal magnetostriction and giant magnetoresistance. The distinctiveness of this series is in the remarkable flexibility of the chemical bonding between well-defined, subnanometer-thick slabs and the resultant magnetic, transport, and thermodynamic properties of these materials. This can be controlled by varying either or both RE and Tt elements, including mixed rare-earth elements on the RE sites and different group 14 (or T = group 13 or 15) elements occupying the Tt sites. In addition to chemical means, the interslab interactions are also tunable by temperature, pressure, and magnetic field. Thus, this system provides a splendid 'playground' to investigate the interrelationships among composition, structure, physical properties, and chemical bonding. The work presented in this dissertation involving RE5T4 materials has resulted in the successful synthesis, characterization, property measurements, and theoretical analyses of various new intermetallic compounds. The results provide significant insight into the fundamental magnetic and structural behavior of these materials and help us better understand the complex link between a compound's composition, its observed structure, and its properties.

  19. Magnetocaloric effect and critical behavior in La0.8-xPrxSr0.2MnO3 (x = 0.2, 0.4, 0.5) manganites

    Science.gov (United States)

    Zarifi, M.; Kameli, P.; Mansouri, M.; Ahmadvand, H.; Salamati, H.

    2017-08-01

    This paper reports on an investigation carried out to determine the effects of Pr substitution on the magnetocaloric and critical behavior of La0.8-xPrxSr0.2MnO3 (x = 0.2, 0.4, 0.5) manganites. Structural studies show that all the compositions are single phase with a rhombohedral structure. Moreover, the lattice parameters and unit cell volume decrease with increasing Pr concentration while the Curie temperature (TC) decreases with Pr3+ substitution for La3+ ions. Arrot's plots are used to determine the nature of the second order magnetic transition; no obvious hysteresis loss is observed in the vicinity of TC in any of the samples. An exhaustive study of the critical behavior of the paramagnetic to ferromagnetic transition is conducted to determine the values of the critical exponents (β, γ, and δ) based on the modified Arrot's plot and using the Kouvel-Fisher method. We have obtained the critical exponents used 3D-Heisenberg and 3D-Ising models. It was found that with increasing Pr doping the values of β and γ decrease and increase, respectively. This suggests an increase in the ferromagnetic short-range order as a result of increasing Pr content in the La0.8-xPrxSr0.2MnO3 samples. Maximum changes in the magnetic entropy were found to be 4.16, 3.88, and 3.8 J kg-1 K-1 under an applied magnetic field of 5 T while the Relative Cooling Power (RCP) values reached 174.7, 252.3, and 255 J kg-1 for x = 0.2, 0.4, and 0.5, respectively.

  20. Efficient Room-Temperature Cooling with Magnets

    NARCIS (Netherlands)

    Boeije, M.F.J.; Roy, P.; Guillou, F.; Yibole, Hargen; Miao, X.F.; Caron, L.; Banerjee, D.; van Dijk, N.H.; de Groot, R.M.; Brück, E.H.

    2016-01-01

    Magnetic cooling is a highly efficient refrigeration technique with the potential to replace the traditional vapor compression cycle. It is based on the magnetocaloric effect, which is associated with the temperature change of a material when placed in a magnetic field. We present experimental

  1. Searching the conditions for a table-like shape of the magnetic entropy in magneto-caloric materials

    Energy Technology Data Exchange (ETDEWEB)

    Álvarez, Pablo, E-mail: pablo.alvarez@ehu.es [Departamento de Electricidad y Electrónica, Universidad del País Vasco (UPV/EHU), 48940 Leioa (Spain); Departamento de Física, Universidad de Oviedo, c/ Calvo Sotelo, s/n, 33007 Oviedo (Spain); Gorria, Pedro, E-mail: pgorria@uniovi.es [Departamento de Física, Universidad de Oviedo, c/ Calvo Sotelo, s/n, 33007 Oviedo (Spain); Sánchez Llamazares, José L. [División de Materiales Avanzados, Instituto Potosino de Investigación Científica y Tecnológica, Camino a la presa San José 2055, CP 78216 San Luis Potosí (Mexico); Blanco, Jesús A. [Departamento de Física, Universidad de Oviedo, c/ Calvo Sotelo, s/n, 33007 Oviedo (Spain)

    2013-08-15

    Highlights: •The magnetic entropy change for two-ribbon (amorphous) composite materials is investigated. •The conditions to obtain a table-like shape of the magnetic entropy change are specified. •We give the essential ingredients to maximize the effective refrigerant capacity and the efficiency. •Our findings could be used in other magneto-caloric materials to tune the temperature range for the table-like behavior. -- Abstract: We show a systematic study of the magneto-caloric response carried out on a series of FeZrB(Cu) amorphous ribbons with different Curie temperature values in the 210–320 K interval. The main aim of the work is to investigate the conditions to obtain, from the isothermal magnetic entropy change vs. temperature curves, ΔS{sub M}(T), a table-like behavior of the entropy using two-ribbon composites. Even though the maximum value of ΔS{sub M} for the composite is lower than those of the single components, the existence of a table-like behavior maximizes the effective refrigerant capacity, reaching values around 80 J/kg for an applied magnetic field change of 2 T. Furthermore, we discuss how the temperature range for such a table-like behavior can be tuned and the refrigerant capacity enhanced in terms of energy efficiency.

  2. Structural, atomic Hirschfeld surface, magnetic and magnetocaloric properties of SmNi{sub 5} compound

    Energy Technology Data Exchange (ETDEWEB)

    Nouri, K., E-mail: nouri@icmpe.cnrs.fr [C.M.T.R, I.C.M.P.E, CNRS, Université Paris Est Créteil, UMR 7182, 2-8 rue Henri Dunant, F-94320 Thiais (France); Laboratoire des Sciences des Matériaux et de l' Environnement, Faculté des Sciences de Sfax- Université de Sfax, BP 1171, Sfax, 3018 (Tunisia); Jemmali, M. [Laboratoire des Sciences des Matériaux et de l' Environnement, Faculté des Sciences de Sfax- Université de Sfax, BP 1171, Sfax, 3018 (Tunisia); Chemistry Departement, College of Science and Arts at Ar-Rass, Qassim University, P.O. Box53 (Saudi Arabia); Walha, S. [Laboratoire des Sciences des Matériaux et de l' Environnement, Faculté des Sciences de Sfax- Université de Sfax, BP 1171, Sfax, 3018 (Tunisia); Zehani, K. [C.M.T.R, I.C.M.P.E, CNRS, Université Paris Est Créteil, UMR 7182, 2-8 rue Henri Dunant, F-94320 Thiais (France); Ben Salah, A. [Laboratoire des Sciences des Matériaux et de l' Environnement, Faculté des Sciences de Sfax- Université de Sfax, BP 1171, Sfax, 3018 (Tunisia); Bessais, L. [C.M.T.R, I.C.M.P.E, CNRS, Université Paris Est Créteil, UMR 7182, 2-8 rue Henri Dunant, F-94320 Thiais (France)

    2016-07-05

    The SmNi{sub 5} intermetallic compound has been investigated by arc-melting. Powder X-ray diffraction analysis and Rietveld refinement revealed that the sample crystallized in the hexagonal CaCu{sub 5}-type structure P6/mmm space group with the following lattice parameters: a = 4.9203 (1) Å, c = 3.9662 (1) Å. These lattice parameters for the compound are in good agreement with previous theoretical result and experimental data. The EDX analysis has been performed to confirm the composition of this compound. The chemical bonding in SmNi{sub 5} was analyzed using atomic Hirshfeld surfaces, and this analysis supports the presence of the structural elements and the coordination of Sm (1a), Ni (2c) and Ni (3 g). This study indicates the different types of interatomic interactions between the Sm and Ni atoms and the weak interactions between Sm–Sm atoms were also observed along the c axis. The magnetic properties and magnetocaloric effect (MCE) have been established by the magnetization and isothermal magnetization of different temperature measurements. The magnetization curve as a function of temperature shows a magnetic transition from ferromagnetic to paramagnetic state at the Curie temperature T{sub C} = 29 K. We have studied the MCE phenomena in the vicinity of magnetic phase transitions in terms of magnetic entropy change. The temperature dependence of the magnetization, the magnetic entropy changeΔS{sub M}, as well as the relative cooling power around the second-order magnetic transition and the Arrott plots for the alloys are reported. - Highlights: • The SmNi{sub 5} intermetallic compound has been investigated by arc-melting. • The chemical bonding in SmNi{sub 5} was analyzed using atomic Hirshfeld surfaces. • The second order magnetocaloric material SmNi{sub 5} is investigated.

  3. Observation of short range ferromagnetic interactions and magnetocaloric effect in cobalt substituted Gd5Si2Ge2.

    Science.gov (United States)

    Uthaman, Bhagya; Manju, P; Thomas, Senoy; Jaiswal Nagar, Deepshikha; Suresh, K G; Varma, Manoj Raama

    2017-05-17

    We report on the observation of double transition - a first order and a second order transition in Gd 5 Si 2-x Co x Ge 2 with x = 0, 0.1, 0.2 and 0.4 with the appearance of short-range ferromagnetic correlations. The first order phase transition is due to a combined magnetostructural transition from monoclinic paramagnetic phase to orthorhombic ferromagnetic phase on cooling while the second order transition arises from an orthorhombic paramagnetic to ferromagnetic phase on cooling. Structural studies show that the substituted compounds crystallize in a combination of Gd 5 Si 2 Ge 2 and Gd 5 Si 4 phases. Low-temperature X-ray diffraction measurements confirm the complete transformation from monoclinic to orthorhombic phase. DC magnetization measurements reveal an anomalous low field magnetic behaviour indicating a Griffiths-like phase. This unusual behaviour is attributed to the local disorder within the crystallographic structure indicating the presence of short-range magnetic correlations and ferromagnetic clustering, which is stabilized and enhanced by competing intra-layer and inter-layer magnetic interactions. The magnetostructural transition results in entropy changes (-ΔS M ) of 9 J kg -1 K -1 at 260 K for x = 0.1, 8.5 J kg -1 K -1 at 245 K for x = 0.2 and 4.2 J kg -1 K -1 at 210 K for x = 0.4 for a field change of 50 kOe. Co substitution induces compelling crystallographic and magnetoresponsive effects in the Gd-Si-Ge system, which could be useful for potential and smart applications such as solid-state magnetic refrigeration and sensitive magnetic switching from paramagnetic to ferromagnetic state. Universal curve analysis has been carried out on the substituted samples to study the order of the magnetic transition.

  4. Adiabatic temperature change from non-adiabatic measurements

    Czech Academy of Sciences Publication Activity Database

    Carvalho, A.M.G.; Mejía, C.S.; Ponte, C.A.; Silva, L.E.L.; Kaštil, Jiří; Kamarád, Jiří; Gomes, A.M.

    2016-01-01

    Roč. 122, č. 3 (2016), s. 1-5, č. článku 246. ISSN 0947-8396 Institutional support: RVO:68378271 Keywords : magnetocaloric effect * adiabatic temperature change * calorimetric device * gadolinium Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 1.455, year: 2016

  5. Quantitative feasibility study of magnetocaloric energy conversion utilizing industrial waste heat

    International Nuclear Information System (INIS)

    Vuarnoz, D.; Kitanovski, A.; Gonin, C.; Borgeaud, Y.; Delessert, M.; Meinen, M.; Egolf, P.W.

    2012-01-01

    Highlights: ► We model magnetic energy conversion machine for the use of industrial waste heat. ► Efficiencies and masses of the system are evaluated by a numerical model. ► Excellent potential of profitability is expected with large low-exergy heat sources. -- Abstract: The main objective of this theoretical study was to investigate under which conditions a magnetic energy conversion device (MECD) – utilizing industrial waste heat – is economically feasible. Furthermore, it was evaluated if magnetic energy conversion (MCE) has the potential of being a serious concurrent to already existing conventional energy conversion technologies. Up-today the availability of magnetocaloric materials with a high Curie temperature and a high magnetocaloric effect is rather limited. Therefore, this study was mainly focused on applications with heat sources of low to medium temperature levels. Magnetic energy conversion machines, containing permanent magnets, are numerically investigated for operation conditions with different temperature levels, defined by industrial waste heat sources and environmental heat sinks, different magnetic field intensities and different frequencies of operation (number of thermodynamic cycles per unit of time). Theoretical modeling and numerical simulations were performed in order to determine thermodynamic efficiencies and the exergy efficiencies as function of different operation conditions. From extracted data of our numerical results, approximate values of the total mass and total volume of magnetic energy conversion machines could be determined. These important results are presented dependent on the produced electric power. An economic feasibility study supplements the scientific study. It shows an excellent potential of profitability for certain machines. The most important result of this article is that the magnetic energy conversion technology can be economically and technically competitive to or even beat conventional energy

  6. Influence of magnetic field, chemical pressure and hydrostatic pressure on the structural and magnetocaloric properties of the Mn-Ni-Ge system

    Science.gov (United States)

    Taubel, Andreas; Gottschall, Tino; Fries, Maximilian; Faske, Tom; Skokov, Konstantin P.; Gutfleisch, Oliver

    2017-11-01

    The magnetic, structural and thermomagnetic properties of the MM’X material system of MnNiGe are evaluated with respect to their utilization in magnetocaloric refrigeration. The effects of separate and simultaneous substitution of Fe for Mn and Si on the Ge site are analysed in detail to highlight the benefits of the isostructural alloying method. A large range of compounds with precisely tunable structural and magnetic properties and the tuning of the phase transition by chemical pressure are compared to the effect of hydrostatic pressure on the martensitic transition. We obtained very large isothermal entropy changes Δ S_iso of up to -37.8 J kg-1 K-1 based on magnetic measurements for (Mn,Fe)NiGe in moderate fields of 2 T. The enhanced magnetocaloric properties for transitions around room temperature are demonstrated for samples with reduced Ge, a resource critical element. An adiabatic temperature change of 1.3 K in a magnetic field change of 1.93 T is observed upon direct measurement for a sample with Fe and Si substitution. However, the high volume change of 2.8% results in an embrittlement of large particles into several smaller fragments and leads to a sensitivity of the magnetocaloric properties towards sample shape and size. On the other hand, this large volume change enables to induce the phase transition with a large shift of the transition temperature by application of hydrostatic pressure (72 K GPa-1 ). Thus, the effect of 1.88 GPa is equivalent to a substitution of 10% Fe for Mn and can act as an additional stimulus to induce the phase transition and support the low magnetic field dependence of the phase transition temperature for multicaloric applications.

  7. Study of magnetocaloric effect in LaFe11∙5Si1∙5 alloys prepared by ...

    Indian Academy of Sciences (India)

    Administrator

    Abstract. LaFe11∙5Si1∙5 alloys are annealed at 1503 K for 5 h and cooled down to room temperature by furnace cooling, air cooling and quenching in ice water, respectively. The main phases are 1:13 phases in those alloys. The impurity phases are α-Fe and the amount of LaFeSi phase is so small that it is hard to observe ...

  8. Phase control studies in Gd{sub 5}Si{sub 2}Ge{sub 2} giant magnetocaloric compound

    Energy Technology Data Exchange (ETDEWEB)

    Belo, J.H. [IFIMUP and IN-Institute of Nanoscience and Nanotechnology, Departamento de Fisica e Astronomia, Faculdade de Ciencias, Universidade do Porto, Rua do Campo Alegre, 687, 4169-007 Porto (Portugal); Pereira, A.M., E-mail: ampereira@fc.up.pt [IFIMUP and IN-Institute of Nanoscience and Nanotechnology, Departamento de Fisica e Astronomia, Faculdade de Ciencias, Universidade do Porto, Rua do Campo Alegre, 687, 4169-007 Porto (Portugal); Ventura, J.; Oliveira, G.N.P. [IFIMUP and IN-Institute of Nanoscience and Nanotechnology, Departamento de Fisica e Astronomia, Faculdade de Ciencias, Universidade do Porto, Rua do Campo Alegre, 687, 4169-007 Porto (Portugal); Araujo, J.P., E-mail: jearaujo@fc.up.pt [IFIMUP and IN-Institute of Nanoscience and Nanotechnology, Departamento de Fisica e Astronomia, Faculdade de Ciencias, Universidade do Porto, Rua do Campo Alegre, 687, 4169-007 Porto (Portugal); Tavares, P.B.; Fernandes, L. [Departamento de Quimica and CQ-VR, Universidade de Tras-os-Montes e Alto Douro, 5001-801 Vila Real (Portugal); Algarabel, P.A. [Instituto de Ciencia de Materiales de Aragon, Universidad de Zaragoza and Consejo Superior de Investigaciones Cientificas, 50009 Zaragoza (Spain); Magen, C. [Instituto de Nanociencia de Aragon-ARAID, Universidad de Zaragoza, 50009 Zaragoza (Spain); Morellon, L. [Instituto de Ciencia de Materiales de Aragon, Universidad de Zaragoza and Consejo Superior de Investigaciones Cientificas, 50009 Zaragoza (Spain); Instituto de Nanociencia de Aragon, Universidad de Zaragoza, 50009 Zaragoza (Spain); and others

    2012-07-15

    Highlights: Black-Right-Pointing-Pointer Study of time dependence of O(I) to M phase. Black-Right-Pointing-Pointer Determination of the optimal annealing time. Black-Right-Pointing-Pointer New method for phase amount estimation (O(I) and M). Black-Right-Pointing-Pointer Effect of annealing on the MCE. Black-Right-Pointing-Pointer Analysis of the nature of the magnetic transition through the Arrot plot representation. - Abstract: A systematic set of annealings on arc-melted synthesized Gd{sub 5}Si{sub 2}Ge{sub 2} sample was performed. Through powder X-ray diffraction (XRD) and magnetometry measurements we monitored the effect of varying the annealing time with constant temperature (T = 1473 K) on the formation of the monoclinic (M) crystallographic phase fraction, which is the one responsible for the giant magnetocaloric effect (GMCE) in this compound. The conversion of the orthorhombic O(I) crystallographic phase into M was achieved, resulting in a significant increase of the M mass fraction. Such conversion led to a change in the magnetic transition nature, evolving from a second to a first order transition for the as-cast and annealed samples, respectively. An optimal annealing time range for the M phase conversion was identified to be within 80-120 min at T = 1473 K followed by a rapid quenching to liquid N{sub 2}. Furthermore, an increase up to {approx}50% of the magnetocaloric effect was obtained for the sample annealed during 120 min.

  9. Magnetocaloric effect and H gradient in bulk La(Fe,Si)13Hy magnetic refrigerants obtained by HDSH

    DEFF Research Database (Denmark)

    Neves Bez, Henrique; Eggert, Bruno G.F.; Lozano, Jaime

    2015-01-01

    the conventional ingot homogenization heat treatment of 7 days. The samples produced by HDSH showed higher amounts of hydrogen than the parts hydrogenated by the conventional method of thermal homogenization (20 h at 1423 K), milling to fine powder and subsequent hydrogenation. Hydrogenation parameters play...... an important role for the stability of the desired La(Fe,Si)13 phase during the process. Hydrogen desorption was seen to occur at two temperature ranges as a result of internal gradients. Dissimilar amounts of α-Fe were precipitated for different hydrogenation times. As a result, parts produced via HDSH with 2...

  10. Materials for room temperature magnetic refrigeration

    Energy Technology Data Exchange (ETDEWEB)

    Rosendahl Hansen, B.

    2010-07-15

    Magnetic refrigeration is a cooling method, which holds the promise of being cleaner and more efficient than conventional vapor-compression cooling. Much research has been done during the last two decades on various magnetic materials for this purpose and today a number of materials are considered candidates as they fulfill many of the requirements for a magnetic refrigerant. However, no one material stands out and the field is still active with improving the known materials and in the search for a better one. Magnetic cooling is based on the magnetocaloric effect, which causes a magnetic material to change its temperature when a magnetic field is applied or removed. For room temperature cooling, one utilizes that the magnetocaloric effect peaks near magnetic phase transitions and so the materials of interest all have a critical temperature within the range of 250 - 310 K. A magnetic refrigerant should fulfill a number of criteria, among these a large magnetic entropy change, a large adiabatic temperature change, preferably little to no thermal or magnetic hysteresis and the material should have the stability required for long term use. As the temperature range required for room temperature cooling is some 40 - 50 K, the magnetic refrigerant should also be able to cover this temperature span either by exhibiting a very broad peak in magnetocaloric effect or by providing the opportunity for creating a materials series with varying transition temperatures. (Author)

  11. Review on numerical modeling of active magnetic regenerators for room temperature applications

    DEFF Research Database (Denmark)

    Nielsen, Kaspar Kirstein; Tusek, Jaka; Engelbrecht, Kurt

    2011-01-01

    . This paper reviews the existing numerical modeling of room temperature AMR to date. The governing equations, implementation of the magnetocaloric effect (MCE), fluid flow and magnetic field profiles, thermal conduction etc. are discussed in detail as is their impact on the AMR cycle. Flow channeling effects...

  12. The influence of quench atomic disorder on the magnetocaloric properties of Ni–Co–Mn–In alloys

    International Nuclear Information System (INIS)

    Singh, Sandeep; Glavatskyy, Illya; Biswas, C.

    2014-01-01

    Highlights: • Large magnetic entropy change (ΔS m = 11 J/Kg K) at 1.5 Tesla above 300 K is obtained. • The peak value of ΔS m is higher in disordered system. • Refrigeration capacity (RC) is unaffected by the quenched atomic disorder. - Abstract: The magnetocaloric effect in Ni–Co–Mn–In alloys is studied at low magnetic field, across the first order magnetostructural transition. The Co doping at Ni site induces the large magnetic entropy change (ΔS m ) above room temperature. The large ΔS m of 11 J/Kg K has been observed for disordered Ni 1.81 Co 0.22 Mn 1.46 In 0.51 alloy at 337 K at an applied field of 1.5 Tesla. The influence of quench atomic disorder on the magnetocaloric properties of Ni–Co–Mn–In alloys has been studied. The atomic disorder significantly increases the peak value of ΔS m and decreases the peak width. The refrigeration capacity (RC) is almost unchanged with atomic disorder

  13. Modelling and simulation of regenerators with complex flow arrangements for active magnetocaloric refrigeration

    DEFF Research Database (Denmark)

    Lei, Tian; Nielsen, Kaspar Kirstein; Engelbrecht, Kurt

    2014-01-01

    Compared to a conventional vapor compression refrigera-tion system, a magnetocaloric refrigerator has many advantages, such as potentially high efficiency, low vibration and avoidance of refrigerants that deplete the ozone layer and cause the green-house effect. As a main component of the active...

  14. Magnetic structure and phase formation of magnetocaloric Mn-Fe-P-X compounds

    NARCIS (Netherlands)

    Ou, Z.Q.

    2013-01-01

    This thesis presents a study of the crystal and magnetic structure, the magnetocaloric effect and related physical properties in Mn-Fe-P-X compounds. The influences of boron addition in (Mn,Fe)2(P,As) compounds have been studied. It is found that boron atoms occupy interstitial sites within the

  15. A new type of magnetocaloric composite based on conductive polymer and magnetocaloric compound

    Energy Technology Data Exchange (ETDEWEB)

    Imamura, W., E-mail: williamimamura@yahoo.com.br [State University of Maringá (UEM)/Department of Mechanical Engineering (DEM-PEM), 87020-900 Maringá, PR (Brazil); Coelho, A.A. [State University of Campinas (Unicamp)/Department of Applied Physics (DFA-IFGW), 13083-859 Campinas, SP (Brazil); Kupfer, V.L. [State University of Maringá (UEM)/Department of Chemistry (DQI-LMSen), 87020-900 Maringá, PR (Brazil); Carvalho, A.M.G. [Brazilian Synchrotron Light Laboratory (LNLS)/Brazilian Center for Research in Energy and Materials (CNPEM), C. P. 6192, 13083-970 Campinas, SP (Brazil); Zago, J.G. [State University of Maringá (UEM)/Department of Mechanical Engineering (DEM-PEM), 87020-900 Maringá, PR (Brazil); Rinaldi, A.W. [State University of Maringá (UEM)/Department of Chemistry (DQI-LMSen), 87020-900 Maringá, PR (Brazil); Favaro, S.L.; Alves, C.S. [State University of Maringá (UEM)/Department of Mechanical Engineering (DEM-PEM), 87020-900 Maringá, PR (Brazil)

    2017-03-01

    We introduce a processing route of the first magnetocaloric composite with conductive polymer – wherein the magnetocaloric reinforcement is a compound Gd{sub 5.09}Ge{sub 2.03}Si{sub 1.88} and the ductile matrix is a conductive polymer polyaniline doped by camphorsulfonic acid (PAni-CSA). This new type of composite combines mechanical, electrical and magnetocaloric properties that can be applied in thermomagnetic machines. - Highlights: • We developed a new type of magnetocaloric composite: PAni-CSA/Gd5.09Ge2.03Si1.88. • We presented a processing route which use a conductive polymer instead of epoxy resins or thermoplastic polymers. • We varied the concentration of PAni-CSA (numerical type) and sintering (categorical type). • We analyzed the matrix (PAni-CSA), the magnetocaloric reinforcement (Gd5.09Ge2.03Si1.88) and the composites. • We presented and discussed mechanical, electrical and magnetocaloric properties.

  16. Magnetostructural transformation and magnetocaloric effect in Ni42Mn47.5Sn10.5 and Ni41.5Mn47.5Sn10.5Zn0.5 ferromagnetic shape memory alloys

    Science.gov (United States)

    Hassan, Najam ul; Shah, Ishfaq Ahmad; Rauf, Abdur; Liu, Jun; Gong, Yuanyuan; Xu, Feng

    2018-02-01

    A comparative investigation on magnetostructural transformation and coupled magnetocaloric properties of Ni42Mn47.5Sn10.5 and Ni41.5Mn47.5Sn10.5Zn0.5 ferromagnetic shape memory alloys prepared by arc-melting method is carried out through structural and magnetic measurements. As Zn is doped in NiMnSn alloy, the cell volume decreases and the martensitic transformation temperature increases by 21 K. Obvious metamagnetic behavior and magnetic hysteresis is observed in isothermal magnetization curves, indicating the magnetic field induced magnetostructural transformation. Magnetic field induced phase transition is also confirmed under applied field of 2 T and martensitic transformation temperature is decreased by 4.1 and 5.29 K for Ni42Mn47.5Sn10.5 and Ni41.5Mn47.5Sn10.5Zn0.5 alloys, respectively. The entropy change in Ni41.5Mn47.5Sn10.5Zn0.5 alloy with change in magnetic field from 0 to 2 T is 12.3 J · kg‑1 · K‑1, which is larger than that in Ni42Mn47.5Sn10.5 alloy. The achieved low field entropy change in Zn doped alloy suggests its potential application as magnetic cooling refrigerant.

  17. Structural characterization, magnetic properties and magnetocaloric effects of La{sub 0.75}Sr{sub 0.25}Mn{sub 1-x}Cr{sub x}O{sub 3} (x = 0.15, 0.20, and 0.25)

    Energy Technology Data Exchange (ETDEWEB)

    Dhahri, A.; Dhahri, E. [Universite de Sfax, Laboratoire de Physique Appliquee, Faculte des Sciences de Sfax (Tunisia); Hlil, E.K. [CNRS et Universite Joseph Fourier, Institut Neel, Grenoble (France)

    2014-09-15

    The effect of Cr doping on the structural, magnetic and magnetocaloric properties of perovskite manganites La{sub 0.75}Sr{sub 0.25}Mn{sub 1-x} Cr{sub x} O{sub 3} (x = 0.15, 0.20, and 0.25) has been investigated. Crystalline structure and magnetic properties are investigated by using X-ray powder diffraction and magnetization measurements, respectively. All samples show a single phase and are found to crystallize in the distorted rhombohedral system with R anti 3c space group. A monotonous change of Curie temperature (T{sub C}), from 314 to 253 K, is observed when content doping increases. Substantial magnetic entropy change reaching 4.20 J/kg K is revealed. Relative cooling power was estimated as well. It was found to reach 289, 323, and 386 J/kg for x = 0.15, 0.20, and 0.25, respectively. Field dependence of the magnetic entropy change showing the power law dependence ΔS{sub M} ∝ (μ{sub 0}H){sup n} is also analyzed and discussed. (orig.)

  18. Developing a Magnetocaloric Domestic Heat Pump

    DEFF Research Database (Denmark)

    Bahl, Christian R.H.

    2014-01-01

    beverage coolers, A/Cs for cars and electronics cooling. Devices for heating have not been extensively demonstrated. Here we consider a promising application of magnetocaloric heat pumps for domestic heating. The task of designing and building such a device is a multidisciplinary one encompassing materials...

  19. Study of magnetic, structural and magnetocaloric properties of La{sub 0.6}Pr{sub 0.4}Mn{sub 2}Si{sub 2} under high pressures and magnetic field

    Energy Technology Data Exchange (ETDEWEB)

    Kaštil, J., E-mail: kastil@fzu.cz [Institute of Physics AS CR v.v.i., Na Slovance 2, 182 21 Prague 8 (Czech Republic); Arnold, Z. [Institute of Physics AS CR v.v.i., Na Slovance 2, 182 21 Prague 8 (Czech Republic); Isnard, O. [Centre national de la recherche scientifique (CNRS), Institut Néel, 25 rus des martyrs, F-38042 Grenoble (France); Université Grenoble Alpes, Institut Néel, F-38042 Grenoble (France); Skourski, Y. [Hochfeld-Magnetlabor Dresden (HLD), HZ Dresden-Rossendorf, D-01314 Dresden (Germany); Kamarád, J. [Institute of Physics AS CR v.v.i., Na Slovance 2, 182 21 Prague 8 (Czech Republic); Itié, J.P. [Synchrotron SOLEIL, L' Orme des Merisiers, Saint-Aubin, 91192 Gif-sur-Yvette (France)

    2017-02-15

    The structural, magnetic and magnetocaloric properties of La{sub 0.6}Pr{sub 0.4}Mn{sub 2}Si{sub 2} compound were measured in wide range of temperature, magnetic field and hydrostatic pressure. The structural study up to 10 GPa confirmed the existence of critical Mn-Mn distance 0.2883 nm for the ferromagnetic to antiferromagnetic transition at room temperature. The results demonstrated the crucial role of the volume in the suppression of the ferromagnetic phase above the transition temperature T{sub 1}=168 K under pressure. The huge pressure shift of the transition temperature T{sub 1}, dT{sub 1}/dp=230 K/GPa, was observed. Based on our magnetization measurement the low temperature transition at T{sub 2}=30 K is connected with reorientation of Mn moment and the rare-earth sublattice is not ordered in this case. The direct magnetocaloric measurement showed moderate values of the adiabatic temperature change connected with the magnetic transition at T{sub c} and T{sub 1} and confirmed the first order character of the transition at T{sub 1} and second order character of the transition at T{sub c}. - Highlights: • The huge pressure shift of the transition temperature dT{sub 1}/dp=230 K/GPa was observed. • Ferromagnetic order is suppressed by applying pressure of 1 GPa. • The direct magnetocaloric effect showed moderate values of ΔT{sub ad}.

  20. Influence of manganite powder grain size and Ag-particle coating on the magnetocaloric effect and the active magnetic regenerator performance

    DEFF Research Database (Denmark)

    Turcaud, J.A.; Neves Bez, Henrique; Ruiz-Trejo, E.

    2015-01-01

    be significantly modified by the Ag-particle coating when the material is examined in sintered pellet form and we compare results with a second manganite composition La0.67Ca0.33MnO3 with significantly smaller grain size. However, we find that this microstructural engineering does not improve the performance...... of the active magnetic regenerator cycle using the silver decorated material in powder form. The regenerator performance is improved by the reduction of the powder grain size of the refrigerant which we attribute to improved thermal management due to increased surface to volume ratio. © 2015 Acta Materialia Inc......The magnetocaloric performance of La0.67Ca0.27Sr0.06Mn1.05O3 is investigated as a function of the powder grain size and also as a function of decoration of grains with highly conductive silver particulates as a coating layer. We demonstrate that the thermal and electrical conductivities can...

  1. Magneto-caloric and magneto-resistive properties of La{sub 0.67}Ca{sub 0.33-x}Sr{sub x}MnO{sub 3}

    Energy Technology Data Exchange (ETDEWEB)

    Reves Dinesen, Anders

    2004-08-01

    This thesis presents results of an experimental investigation of magneto-caloric and magneto-resistive properties of a series of polycrystalline Ca- and Sr-doped lanthanum manganites, La{sub 0.67}Ca{sub 0.33-x}Sr{sub x}MnO{sub 3} (0{<=} x {<=} 0.33), with the perovskite structure. The samples consisted of sintered oxide powders prepared the glycine-nitrate combustion technique. The compounds were ferromagnetic and showed a Curie transition in the temperature range 267370 K (T{sub C} increased with increasing x). An analysis of the structural properties was carried out by means of x-ray diffraction and the Rietveld technique. The variation of the Ca/Sr ratio was found to cause a transition from orthorhombic to rhombohedral symmetry in the composition range 0.110 < x < 0.165. The analysis suggested a strong correlation between structural properties and magnetism, for instance a relationship between the mean MnOMn bond angle and the Curie temperature. The MnOMn bonds mediate ferromagnetism and electrical transport in these materials via the double-exchange mechanism. The magnetocaloric effect of the La{sub 0.67}Ca{sub 0.33-x}Sr{sub x}MnO{sub 3} samples was measured directly and indirectly (by means of magnetization measurements). All the samples showed a magnetocaloric effect in the vicinity of T{sub C}. A model for the mag-netocaloric effect based on Weiss mean field theory and classical theories for heat capacities was developed. The model provided reasonable predictions of the magneto-caloric properties of the samples. The compounds with low Sr content showed a magnetocaloric effect comparable to that of Gadolinium, the prototypical working material for magnetic refrigeration at room temperature. A less comprehensive part of the investigation regarded the magneto-resistive properties of the La{sub 0.67}Ca{sub 0.33-x}Sr{sub x}MnO{sub 3} system. It was found that th polycrystalline nature of the compounds played a decisive role for the magnetotransport properties

  2. Thermomagnetic and magnetocaloric properties of metamagnetic Ni-Mn-In-Co Heusler alloy in magnetic fields up to 140 kOe

    Directory of Open Access Journals (Sweden)

    Kamantsev Alexander

    2014-07-01

    Full Text Available High cooling power of magnetocaloric refrigeration can be achieved only at large amounts of heat, which can be transferred in one cycle from cold end hot end at quasi-isothermal conditions. The simple and robust experimental method of direct measuring of the transferred heat of materials with magnetocaloric effect (MCE in thermal contact with massive copper block with definite heat capacity in quasi-isothermal regime was proposed. The vacuum calorimeter for the specific transferred heat ΔQ and adiabatic temperature change ΔT measurements of MCE materials in the fields of Bitter coil magnet up to H = 140 kOe was designed and tested on samples of Ni43Mn37.9In12.1Co7 Heusler alloy with inverse MCE in the vicinity of meta-magnetostructural phase transition (PT. It was found, that the magnetic field H = 80 kOe produces complete PT from martensite to austenite with ΔQ = - 1600 J/kg at initial temperature 273 K.

  3. Modulation infrared thermometry of caloric effects at up to kHz frequencies

    Science.gov (United States)

    Döntgen, Jago; Rudolph, Jörg; Waske, Anja; Hägele, Daniel

    2018-03-01

    We present a novel non-contact method for the direct measurement of caloric effects in low volume samples. The adiabatic temperature change ΔT of a magnetocaloric sample is very sensitively determined from thermal radiation. Rapid modulation of ΔT is induced by an oscillating external magnetic field. Detection of thermal radiation with a mercury-cadmium-telluride detector allows for measurements at field frequencies exceeding 1 kHz. In contrast to thermoacoustic methods, our method can be employed in vacuum which enhances adiabatic conditions especially in the case of small volume samples. Systematic measurements of the magnetocaloric effect as a function of temperature, magnetic field amplitude, and modulation frequency give a detailed picture of the thermal behavior of the sample. Highly sensitive measurements of the magnetocaloric effect are demonstrated on a 2 mm thick sample of gadolinium and a 60 μm thick Fe80B12Nb8 ribbon.

  4. Magnetocaloric properties of a frustrated Blume-Capel antiferromagnet

    Directory of Open Access Journals (Sweden)

    Žukovič Milan

    2014-07-01

    Full Text Available Low-temperature magnetization processes and magnetocaloric properties of a geometrically frustrated spin-1 Blume-Capel model on a triangular lattice are studied by Monte Carlo simulations. The model is found to display qualitatively different behavior depending on the sign of the single-ion anisotropy D. For positive values of D we observe two magnetization plateaus, similar to the spin-1/2 Ising antiferromagnet, and negative isothermal entropy changes for any field intensity. For a range of small negative values of D there are four magnetization plateaus and the entropy changes can be either negative or positive, depending on the field. If D is negative but large in absolute value then the entropy changes are solely positive.

  5. Investigation on the magnetocaloric effect in DyNi{sub 2}, DyAl{sub 2} and Tb{sub 1-n}Gd{sub n}Al{sub 2} (n=0, 0.4, 0.6) compounds

    Energy Technology Data Exchange (ETDEWEB)

    Sousa, V.S.R. de [Instituto de Fisica Armando Dias Tavares, Universidade do Estado do Rio de Janeiro, Rua Sao Francisco Xavier 524, 20550-900 Rio de Janeiro (Brazil)], E-mail: vinidesousa@gmail.com; Plaza, E.J.R. [Instituto de Fisica Armando Dias Tavares, Universidade do Estado do Rio de Janeiro, Rua Sao Francisco Xavier 524, 20550-900 Rio de Janeiro (Brazil); Reis, M.S. [CICECO, Universidade de Aveiro, 3810-193 Aveiro (Portugal); Alho, B.P. [Instituto de Fisica Armando Dias Tavares, Universidade do Estado do Rio de Janeiro, Rua Sao Francisco Xavier 524, 20550-900 Rio de Janeiro (Brazil); Carvalho, A. Magnus G. [Divisao de Metrologia de Materiais, Inmetro, Duque de Caxias (Brazil); Gama, S. [Departamento de Ciencias Exatas e da Terra, Unifesp, Diadema (Brazil); Oliveira, N.A. de; Ranke, P.J. von [Instituto de Fisica Armando Dias Tavares, Universidade do Estado do Rio de Janeiro, Rua Sao Francisco Xavier 524, 20550-900 Rio de Janeiro (Brazil)

    2009-10-15

    The magnetocaloric effect (MCE) in the DyNi{sub 2}, DyAl{sub 2} and Tb{sub 1-n}Gd{sub n}Al{sub 2} (n=0, 0.4, 0.6) was theoretically investigated in this work. The DyNi{sub 2} and DyAl{sub 2} compounds are described considering a model Hamiltonian which includes the crystalline electrical field anisotropy. The anisotropic MCE was calculated changing the magnetic field direction from <1 1 1> to <0 0 1> in DyNi{sub 2} and from <1 0 0> to <0 1 1> in DyAl{sub 2}. The influence of the second- and first-order spin-reorientation phase transitions on the MCE that occurs in these systems is discussed. For the calculations of the MCE thermodynamic quantities in the Tb{sub 1-n}Gd{sub n}Al{sub 2} systems we take into account a two sites magnetic model, and good agreement with the available experimental data was obtained.

  6. Tunable magnetocaloric effect in Sr{sub 1-x}Ca{sub x}Mn{sub 0.5}Ti{sub 0.5}O{sub 3} perovskites

    Energy Technology Data Exchange (ETDEWEB)

    Shanmugapriya, K.; Palanivel, Balan [Pondicherry Engineering College, Department of Physics, Puducherry (India); Radheep, D.M.; Murugan, Ramaswamy [Pondicherry University, Department of Physics, Puducherry (India)

    2017-07-15

    Sr{sub 1-x}Ca{sub x}Mn{sub 0.5}Ti{sub 0.5}O{sub 3} (x = 0.25, 0.5 and 0.75) polycrystalline samples were synthesized by conventional solid-state reaction. Magnetic characterizations of Sr{sub 1-x}Ca{sub x}Mn{sub 0.5}Ti{sub 0.5}O{sub 3} revealed signature of antiferromagnetic ordering at temperatures (T{sub N}) ∝ 19, 25 and 29.5 K for x = 0.25, x = 0.5 and for x = 0.75, respectively. Sr{sub 1-x}Ca{sub x}Mn{sub 0.5}Ti{sub 0.5}O{sub 3} (x = 0.75) exhibits field-induced antiferromagnetic to ferromagnetic transition at ∝ 30 K with applied magnetic field of 4 and 5 T. Magnetocaloric change (ΔS{sub M}) increases from 3.5 to 19 J/kg K by increasing calcium concentration in the A-site. Those ΔS{sub M} values are relatively very high in these classes of antiferromagnetic perovskite systems and equal to the magnetisation values of the ferromagnetic perovskite manganites. This is the first report for the Sr{sub 1-x}Ca{sub x}Mn{sub 0.5}Ti{sub 0.5}O{sub 3} (x = 0.75) having large magnetic entropy changes induced by the low magnetic field. (orig.)

  7. Magnetocaloric and magnetoelastic effects in (Tb.sub.0.45./sub.Dy.sub.0.55./sub.).sub.1-x./sub.Er.sub.x./sub.Co.sub.2./sub. multicomponent compounds

    Czech Academy of Sciences Publication Activity Database

    Tereshina, I.; Politova, G.; Tereshina, Evgeniya; Nikitin, S.; Burkhanov, G.; Chistyakov, O.; Karpenkov, A.

    2010-01-01

    Roč. 200, č. 9 (2010), 092012/1-092012/5 ISSN 1742-6588. [International Conference on Magnetism - ICM 2009. Karlsruhe, 26.07.2009-31.07.2009] Institutional research plan: CEZ:AV0Z10100520 Keywords : Laves phases * magnetocalorics * magnetostriction Subject RIV: BM - Solid Matter Physics ; Magnetism

  8. Nucleation and dynamics of the metamagnetic transition in magnetocaloric La(Fe,Mn,Si)13

    Science.gov (United States)

    Lovell, E.; Bratko, M.; Caplin, A. D.; Cohen, L. F.

    2017-10-01

    Refrigeration cycle rates of the order of 15 Hz are desirable for efficient solid state based magnetocaloric cooling, placing an upper bound on the combined magnetic transition and the heat transfer times of the order of tens of msecs. We use microcalorimetry and magnetometry to probe the transition dynamics as a function of magnetic field sweep-rate, sample size, thermal environment, temperature and hydrostatic pressure in LaFe11.74Mn0.06Si1.20. Although second order caloric materials follow the magnetisation or demagnetisation driving field without lag, here we show that the field driven evolution of the first-order phase transition in La(Fe,Si)13-based compounds show temporal dynamics on timescales that are significantly longer than tens of msecs, associated with the thermal linkage within the sample and the linkage to the external bath. We observe that features associated with the first nucleation of the transition are field sweep rate independent, and from measurements of the latent heat we infer that the barriers to magnetisation and demagnetisation are of different magnitude. Increasing the temperature or applying hydrostatic pressure reduces the dynamic effects, suggestive of diminishing first-order character of the transition under these conditions.

  9. Magnetic and magnetocaloric properties of spin-glass material DyNi{sub 0.67}Si{sub 1.34}

    Energy Technology Data Exchange (ETDEWEB)

    Chen, X. [The Ames Laboratory, U.S. Department of Energy, Iowa State University, Ames, IA 50011-3020 (United States); College of Physics and Electronic Information Engineering, Neijiang Normal University, Neijiang 641100 (China); Mudryk, Y., E-mail: slavkomk@ameslab.gov [The Ames Laboratory, U.S. Department of Energy, Iowa State University, Ames, IA 50011-3020 (United States); Pathak, A.K.; Feng, W. [The Ames Laboratory, U.S. Department of Energy, Iowa State University, Ames, IA 50011-3020 (United States); Pecharsky, V.K. [The Ames Laboratory, U.S. Department of Energy, Iowa State University, Ames, IA 50011-3020 (United States); Department of Materials Science and Engineering, Iowa State University, Ames, IA 50011-2300 (United States)

    2017-08-15

    Highlights: • Spin-glass state is observed in the DyNi{sub 0.67}Si{sub 1.4} compound. • Random Ni/Si distribution in the AlB{sub 2}-type structure leads to magnetic frustration. • Magnetic frustration affects magnetic field dependence of magnetocaloric effect. - Abstract: Structural, magnetic, and magnetocaloric properties of DyNi{sub 0.67}Si{sub 1.34} were investigated using X-ray powder diffraction, magnetic susceptibility, and magnetization measurements. X-ray powder diffraction pattern shows that DyNi{sub 0.67}Si{sub 1.34} crystallizes in the AlB{sub 2}-type hexagonal structure (space group: P6/mmm, No. 191, a = b = 3.9873(9) Å, and c = 3.9733(1) Å). The compound is a spin-glass with the freezing temperature T{sub G} = 6.2 K. The ac magnetic susceptibility measurements confirm magnetic frustration in DyNi{sub 0.67}Si{sub 1.34}. The maximum value of the magnetic entropy change determined from M(H) data is −16.1 J/kg K at 10.5 K for a field change of 70 kOe.

  10. Effect of Fe substitution on structural, magnetic and magnetocaloric properties of nanocrystalline La0.7Te0.3Mn1-xFexO3 (x=0.1, 0.3)

    Science.gov (United States)

    Meenakshi; Kumar, Amit; Mahato, Rabindra Nath

    2017-04-01

    Structural, magnetic and magnetocaloric properties of the nanocrystalline La0.7Te0.3Mn1-xFexO3 (x=0.1 and 0.3) perovskite manganites were investigated prepared by the sol-gel method. X-ray diffraction indicates that the samples crystallize in rhombohedral crystal structure with R 3 ̅c space group for x=0.1 and orthorhombic structure with Pbnm space group for x=0.3. The average crystallite sizes were calculated using Debye Scherer's formula and were found to be 31 nm and 26 nm for La0.7Te0.3Mn0.90Fe0.1O3 and La0.7Te0.3Mn0.7Fe0.3O3 samples, respectively. The scanning electron microscopy images confirm the homogeneity of the nanocrystalline samples. Temperature dependence magnetization measurements revealed a decrease of ferromagnetic-paramagnetic phase transition with increasing Fe-content. The Curie temperature (TC) determined for x=0.1 and 0.3 are 171 K and 78 K, respectively. Based on the magnetic field dependence of magnetization, M(H), the magnetic entropy change |ΔSM| of the samples were calculated. The maximum entropy change |ΔSmax| values are 1.17 Jkg-1 K-1 for x=0.1 and 0.44 Jkg-1 K-1 for x=0.3 for a field change of 2 T. The relative cooling power was found to be 80 JK-1 and 49 JK-1 for the La0.7Te0.3Mn0.90Fe0.1O3 and La0.7Te0.3Mn0.7Fe0.3O3 samples, which are comparable to other manganites. Tuning of TC with Fe substitution on Mn-site and moderate magnetic entropy change and RCP values, as well as high stability, enable La0.7Te0.3Mn1-xFexO3 (x=0.1 and 0.3) nanocrystalline manganites to be a competitive candidate among the magnetic refrigeration materials for wide temperature ranges from room temperature down to 50 K.

  11. Co and In doped Ni-Mn-Ga magnetic shape memory alloys: a thorough structural, magnetic and magnetocaloric study

    Czech Academy of Sciences Publication Activity Database

    Fabbrici, S.; Porcari, G.; Cugini, F.; Solzi, M.; Kamarád, Jiří; Arnold, Zdeněk; Cabassi, R.; Albertini, F.

    2014-01-01

    Roč. 16, č. 4 (2014), s. 2204-2222 ISSN 1099-4300 Institutional support: RVO:68378271 Keywords : magnetic shape memory materials * magnetocaloric effect * multifunctional Heusler alloys Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 1.502, year: 2014

  12. Rotating disk atomization of Gd and Gd-Y for hydrogen liquefaction via magnetocaloric cooling

    Energy Technology Data Exchange (ETDEWEB)

    Slinger, Tyler [Iowa State Univ., Ames, IA (United States)

    2016-12-17

    In order to enable liquid hydrogen fuel cell technologies for vehicles the cost of hydrogen liquefaction should be lowered. The current method of hydrogen liquefaction is the Claude cycle that has a figure of merit (FOM) of 0.3-0.35. New magnetocaloric hydrogen liquefaction devices have been proposed with a FOM>0.5, which is a significant improvement. A significant hurdle to realizing these devices is the synthesis of spherical rare earth based alloy powders of 200μm in diameter. In this study a centrifugal atomization method that used a rotating disk with a rotating oil quench bath was developed to make gadolinium and gadolinium-yttrium spheres. The composition of the spherical powders included pure Gd and Gd0.91Y0.09. The effect of atomization parameters, such as superheat, melt properties, disk shape, disk speed, and melt system materials and design, were investigated on the size distribution and morphology of the resulting spheres. The carbon, nitrogen, and oxygen impurity levels also were analyzed and compared with the magnetic performance of the alloys. The magnetic properties of the charge material as well as the resulting powders were measured using a vibrating sample magnetometer. The saturation magnetization and Curie temperature were the target properties for the resulting spheres. These values were compared with measurements taken on the charge material in order to investigate the effect of atomization processing on the alloys.

  13. Tunable magnetic and magnetocaloric properties of La0.6Sr0.4MnO3 nanoparticles

    Science.gov (United States)

    Ehsani, M. H.; Kameli, P.; Ghazi, M. E.; Razavi, F. S.; Taheri, M.

    2013-12-01

    Nanoparticles of La0.6Sr0.4MnO3 with different particle sizes are synthesized by the nitrate-complex auto-ignition method. The structural and magnetic properties of the samples are investigated by X-Ray diffraction (XRD), Fourier transform infra-red (FT-IR) spectroscopy, transmission electron microscopy (TEM), and DC magnetization measurements. The XRD study coupled with the Rietveld refinement shows that all samples crystallize in a rhombohedral structure with the space group of R-3 C. The FT-IR spectroscopy and TEM images indicate formation of the perovskite structure with the average sizes of 20, 40, and 100 nm for the samples sintered at 700, 800, and 1100 °C, respectively. The DC magnetization measurements confirm tuning of the magnetic properties due to the particle size effects, e.g., reduction in the ferromagnetic moment and increase in the surface spin disorder by decreasing the particle size. The magnetocaloric effect (MCE) study based on isothermal magnetization vs. filed measurements in all samples reveals a relatively large MCE around the Curie temperature of the samples. The peak around the Curie temperature gradually broadens with reduction of the particle size. The data obtained show that although variations in the magnetic entropy and adiabatic temperature decrease by lowering the particle size, variation in the relative cooling power values are the same for all samples. These results make this material a proper candidate in the magnetic refrigerator application above room temperature at moderate fields.

  14. Magnetic and magnetocaloric properties of amorphous Y{sub 3}Fe{sub 5}O{sub 12} compound

    Energy Technology Data Exchange (ETDEWEB)

    Nóbrega, E.P., E-mail: pilad@cbpf.br; Costa, S.S.; Alvarenga, T.S.T.; Alho, B.P.; Caldas, A.; Ribeiro, P.O.; Sousa, V.S.R de; Oliveira, N.A. de; Ranke, P.J. von

    2017-01-15

    We report a theoretical model formed by two coupled magnetic sublattices of localized spins in the presence of an applied magnetic field to investigate the magnetic characteristics and magnetocaloric properties of amorphous yttrium iron garnet. The magnetic state equation is based on Handrich–Kobe´s theory, where the amorphization is taken into account by introducing fluctuations in the exchange parameters. Experimental results report that Y{sub 3}Fe{sub 5}O{sub 12} presents a structural phase transition from crystalline to amorphous caused by a variation of external pressure. This phase transition on Y{sub 3}Fe{sub 5}O{sub 12} leads to interesting results in the magnetic properties and magnetocaloric quantities. - Highlights: • Study of magnetic and magnetocaloric properties of amorphous Y{sub 3}Fe{sub 5}O{sub 12} compound. • Theoretical model formed by two coupled magnetic sublattices of localized spins in the presence of an applied magnetic field. • The influence of crystalline/amorphous transition on the magnetocaloric effect.

  15. Effect of Co substitution on the physicochemical properties of La0 ...

    Indian Academy of Sciences (India)

    Sol–gel; X-ray diffraction; neutron diffraction; Curie temperature; magnetocaloric effect. 1. Introduction. The term 'manganite' is commonly used to name REMnO3. (RE = trivalent rare-earth ion such as La, Nd and Pr) oxides with ABO3 perovskite structure. Hole doping is achieved by substituting divalent cations at the RE-site ...

  16. Influence of Fe doped on the magnetocaloric behavior of La_{{2}/{3}} Ca_{{1}/{3}} Mn1‑x Fe x O3 compounds: a Monte Carlo simulation

    Science.gov (United States)

    Alzate-Cardona, J. D.; Barco-Rios, H.; Restrepo-Parra, E.

    2018-02-01

    The magnetocaloric behavior of La{2/{3}} Ca{1/{3}} Mn1‑x Fe x O3 for x  =  0.00, 0.02, 0.03, 0.05, 0.07, 0.08 and 0.10 under the influence of an external magnetic field was simulated and analyzed. Simulations were carried out using the Monte Carlo method and the classical Heisenberg model under the Metropolis algorithm. These mixed valence manganites are characterized by having three types of magnetic ions corresponding to Mn4+≤ft(S=\\frac{3}{2}\\right) , which are bonded with Ca2+ , and Mneg3+ and Mneg\\prime3+ (S=2) , related to La3+ . The Fe ions were randomly included, replacing Mn ions. With this model, the magnetic entropy change, Δ S , in an isothermal process was determined. -Δ Sm showed maximum peaks around the paramagnetic-ferromagnetic transition temperature, which depends on Fe doping. Relative cooling power was computed for different Fe concentrations varying the magnetic applied field. Our model and results show that the Fe doping decreases the magnetocaloric effect in the La{2/{3}} Ca{1/{3}} Mn1‑x Fe x O3, making this a bad candidate for magnetic refrigeration. The strong dependence of the magnetocaloric behavior on Fe doping and the external magnetic field in La{2/{3}} Ca{1/{3}} Mn1‑x Fe x O3 can boost these materials for the future technological applications.

  17. Performance-oriented Analysis of a Hybrid magnetic Assembly for a Heat-pump Magnetocaloric Device

    DEFF Research Database (Denmark)

    Insinga, Andrea Roberto; Smith, Anders; Bahl, Christian R.H.

    2014-01-01

    Conventional active-regenerator magnetocaloric devices include moving parts, with the purpose of generating an oscillating magnetic field in the magneto-caloric material, placed inside the regenerator. In this work a different design is analyzed, for application in a magnetocaloric heat pump...

  18. Magnetocaloric Properties of Fe-Ni-Cr Nanoparticles for Active Cooling

    Science.gov (United States)

    Chaudhary, V.; Ramanujan, R. V.

    2016-10-01

    Low cost, earth abundant, rare earth free magnetocaloric nanoparticles have attracted an enormous amount of attention for green, energy efficient, active near room temperature thermal management. Hence, we investigated the magnetocaloric properties of transition metal based (Fe70Ni30)100-xCrx (x = 1, 3, 5, 6 and 7) nanoparticles. The influence of Cr additions on the Curie temperature (TC) was studied. Only 5% of Cr can reduce the TC from ~438 K to 258 K. These alloys exhibit broad entropy v/s temperature curves, which is useful to enhance relative cooling power (RCP). For a field change of 5 T, the RCP for (Fe70Ni30)99Cr1 nanoparticles was found to be 548 J-kg-1. Tunable TCin broad range, good RCP, low cost, high corrosion resistance and earth abundance make these nanoparticles suitable for low-grade waste heat recovery as well as near room temperature active cooling applications.

  19. Cepheid radii and effective temperatures

    International Nuclear Information System (INIS)

    Fernley, J.A.; Skillen, I.; Jameson, R.F.

    1989-01-01

    New infrared photometry for the Cepheid variables T Vul, δ Cephei and XCyg is presented. Combining this with published infrared photometry of T Vul, ηAql, S Sge and XCyg and published optical photometry we use the infrared flux method to determine effective temperatures and angular radii at all phases of the pulsation cycle. These angular radii combined with published radial velocity curves then give the radii of the stars. Knowing the radii and effective temperatures we obtain the absolute magnitudes. (author)

  20. Achieving a table-like magnetocaloric effect and large refrigerant capacity in in situ multiphase Gd65Mn25Si10 alloys obtained by crystallization treatment

    International Nuclear Information System (INIS)

    Shen, X Y; Zhong, X C; Huang, X W; Mo, H Y; Feng, X L; Liu, Z W; Jiao, D L

    2017-01-01

    In situ multiphase structure Gd 65 Mn 25 Si 10 alloys were fabricated by melt spinning and subsequent crystallization treatment. In the process of crystallization, the α -Gd, GdMn 2 and Gd 5 Si 3 phases precipitate in the amorphous matrix in turn. The Curie temperature ( T C ) values for the α -Gd crystallization phase and amorphous matrix can be tailored by tuning the crystallization treatment time. All three multiphase alloys obtained by crystallization treatment at 637 K for 20, 30 and 40 min, respectively, undergo multiple successive magnetic phase transitions. A table-like magnetic entropy change over a wide temperature range (∼90–120 K) and a large full width at half maximum (Δ T FWHM ) magnetic entropy change (∼230 K) were achieved in the above-mentioned crystallized alloys, resulting in large refrigerant capacities (RCs). The enhanced RCs of the three crystallized alloys for a magnetic field change of 0–5 T are in the range of 541–614 J kg −1 . Large Δ T FWHM and RC values and a table-like (−Δ S M ) max feature obtained in in situ multiphase Gd 65 Mn 25 Si 10 crystallized alloys make them suitable for potential application in efficient Ericsson-cycle magnetic refrigeration working in a temperature range from 74 to 310 K. (paper)

  1. Impact of Annealing Temperature on the Physical Properties of the Lanthanum Deficiency Manganites

    Directory of Open Access Journals (Sweden)

    Skini Ridha

    2017-10-01

    Full Text Available The lanthanum deficiency manganites La0.8-x□xCa0.2MnO3 (x = 0, 0.1 and 0.2, where □ is a lanthanum vacancy, were prepared using the classic ceramic methods with different thermal treatments (1373 K and 973 K. The structural, magnetic, and magnetocaloric properties of these compounds were studied as a function of annealing temperature. It was noted that the annealing temperature did not affect the crystal structure of our samples (orthorhombic structure with Pnma space group. Nevertheless, a change in the variation of the unit cell volume V, the average bond length dMn–O, and the average bond angles θMn–O–Mn were observed. Magnetization versus temperature study has shown that all samples exhibited a magnetic transition from ferromagnetic (FM to paramagnetic (PM phase with increasing temperature. However, it can be clearly seen that the annealing at 973 K induced an increase of the magnetization. In addition, the magnetocaloric effect (MCE as well as the relative cooling power (RCP were estimated. As an important result, the values of MCE and RCP in our Lanthanum-deficiency manganites are reported to be near to those found in gadolinium, considered as magnetocaloric reference material.

  2. Long-range ferromagnetism and magnetocaloric effects in rapidly quenched Ni50−xCoxMn50−yAly ribbons

    Directory of Open Access Journals (Sweden)

    Nguyen Thi Mai

    2017-03-01

    Full Text Available Ni50−xCoxMn50−yAly (x = 7 and 9; y = 17, 18 and 19 alloy ribbons were prepared by melt-spinning with a tangential velocity of copper wheel of 40 m s−1. X-ray diffraction patterns reveal multi-crystalline phase behavior in the fabricated ribbons. The shape of thermomagnetization curves clearly depends on Co and Al concentrations. The Curie temperatures (TC of the alloy ribbons strongly increase with increasing the Co concentration and slightly decrease with increasing the Al concentration. The martensitic-austenitic phase transition in the alloy ribbons can be manipulated by tuning Co and Al concentrations. The maximum magnetic entropy change |ΔSm|max of about 0.75 J kg−1 K−1 for a field change of 12 kOe at TC ≈ 364 K was achieved for the Ni43Co7Mn32Al18 ribbon. Critical analysis using the Arrott-Noaks and Kouvel–Fisher methods demonstrates the existence of a long-range ferromagnetic order in this ribbon.

  3. Structure and magnetocaloric properties of La1-xKxMnO3 manganites

    International Nuclear Information System (INIS)

    Aliev, A.M.; Gamzatov, A.G.; Batdalov, A.B.; Mankevich, A.S.; Korsakov, I.E.

    2011-01-01

    A technology of obtaining the single-phase ceramic samples of La 1-x K x MnO 3 manganites and the dependence of their structural parameters on the content of potassium has been described. Magnetocaloric effect (MCE) in the obtained samples has been measured by two independent methods: classical direct methodic and a method of magnetic field modulation. The values of MCE obtained by both methods substantially differ. The explanation of the observed divergences is given. The correlation between the level of doping and MCE value has been defined. The value of T C determined by the MCE maximum conforms with the literature data obtained by other methods.

  4. Modelling and simulation of regenerators with complex flow arrangements for active magnetocaloric refrigeration

    DEFF Research Database (Denmark)

    Lei, Tian; Nielsen, Kaspar Kirstein; Engelbrecht, Kurt

    2014-01-01

    Compared to a conventional vapor compression refrigera-tion system, a magnetocaloric refrigerator has many advantages, such as potentially high efficiency, low vibration and avoidance of refrigerants that deplete the ozone layer and cause the green-house effect. As a main component of the active...... magnetic re-generative refrigerator, the regenerator plays an important role in the cooling performance and efficiency of the whole system. However, the regenerator design is constrained by several exter-nal factors, such as the geometry of the magnetic field source and flow resistance. In this work, novel...

  5. Toward a better understanding of the magnetocaloric effect: An experimental and theoretical study of MnFe.sub.4./sub.Si.sub.3./sub..

    Czech Academy of Sciences Publication Activity Database

    Gourdon, O.; Gottschlich, G.; Persson, J.; de la Cruz, C.; Petříček, Václav; McGuire, M.A.; Bruckel, T.

    2014-01-01

    Roč. 216, AUG (2014), s. 56-64 ISSN 0022-4596 Grant - others:AV ČR(CZ) Praemium Academiae Institutional support: RVO:68378271 Keywords : magneto caloric effect materials * intermetallic * silicide * magnetism * neutron diffraction * density functional theory Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 2.133, year: 2014

  6. The persistence of the magnetocaloric effect in (La1-x)A(x)(0.67)Ba0.33Mn1.05O3-δ

    DEFF Research Database (Denmark)

    Ancona-Torres, Carlos Eugenio; Pryds, Nini; Kuhn, Luise Theil

    2010-01-01

    Polycrystalline samples of (La1-xAx)0.67Ba0.33Mn1.05O3-δ, with A being a mixture of lanthanides containing 66% La, 22% Nd, 8% Pr and 4% Ce, were prepared by the glycine-nitrate method, with target compositions of x = 0, 0.33, 0.67 and 1. The effect of the mixture of lanthanides on the Curie...

  7. Phase analysis and magnetocaloric properties of Zr substituted Gd-Si-Ge alloys

    International Nuclear Information System (INIS)

    Prabahar, K.; Raj Kumar, D.M.; Manivel Raja, M.; Chandrasekaran, V.

    2011-01-01

    The structure, microstructure, magneto-structural transition and magnetocaloric effect have been investigated in series of (Gd 5-x Zr x )Si 2 Ge 2 alloys with 0≤x≥0.20. X-ray powder diffraction analysis revealed the presence of orthorhombic structure for Zr containing alloys at room temperature in contrast to the monoclinic structure observed in the parent Gd 5 Si 2 Ge 2 alloy. The microstructural studies reveal that, low Zr addition (x≤0.1) resulted in low volume fraction of detrimental Gd 5 Si 3 -type secondary phase compared to that present in the parent alloy. All the Zr containing alloys have shown the presence of only second order magnetic transition unlike the parent alloy showing both first order structural and second order magnetic transition. A moderate (ΔS) M value of -5.5 J/kg K was obtained for the x=0.05 alloy at an enhanced operating temperature of 292 K compared to -7.8 J/kg K at 274 K of the parent alloy for an applied field of 2 T. The interesting feature of Zr (x=0.05) containing alloy is the wide operating temperature range of ∼25 K than that of ∼10-12 K for the parent, which resulted in enhanced net refrigerant capacity of 103 J/kg compared to that of 53 J/kg for the parent alloy. - Research highlights: → Zr addition in Gd 5 Si 2 Ge 2 alloy has been investigated for the first time to reduce the 5:3-type (Gd 5 Si 3 ) secondary phase formed when using commercial grade elements in Gd 5 Si 2 Ge 2 alloy. → It is interesting to observe that Zr addition decrease the volume fraction 5:3. → The refrigerator capacity and transition temperature of Zr added alloy is greater than the pure Gd 5 Si 2 Ge 2 which makes this alloy promising for room temperature application.

  8. Tuning the magnetocaloric properties of La0.7Ca0.3MnO3 manganites through Ni-doping

    Science.gov (United States)

    Gómez, A.; Chavarriaga, E.; Supelano, I.; Parra, C. A.; Morán, O.

    2018-04-01

    The effect of Ni2+ doping on the magnetic and magnetocaloric properties of La0.7Ca0.3MnO3 manganites synthesized via the auto-combustion method is reported. The aim of studying Ni2+-substituted La0.7Ca0.3Mn1 - xNixO3 (x = 0 , 0.02 , 0.07, and 0.1) manganites was to explore the possibility of increasing the operating temperature range for the magnetocaloric effect through tuning of the magnetic transition temperature. X-ray diffraction analysis confirmed the phase purity of the synthesized samples. The substitution of Mn3+ ions by Ni2+ ions in the La0.7Ca0.3MnO3 lattice was also corroborated through this technique. The dependence of the magnetization on the temperature reveals that all the compositions exhibit a well-defined ferromagnetic to paramagnetic transition near the Curie temperature. A systematic decrease in the values of the Curie temperature is clearly observed upon Ni2+ doping. Probably the replacement of Mn3+ by Ni2+ ions in the La0.7Ca0.3MnO3 lattice weakens the Mn3+-O-Mn4+ double exchange interaction, which leads to a decrease in the transition temperature and the magnetic moment in the samples. By using Arrott plots, it was found that the phase transition from ferromagnetic to paramagnetic is second order. The maximum magnetic entropy changes observed for the x = 0 , 0.02 , 0.07, and 0.1 composites was 0.85, 0.77, 0.63, and 0.59 J/kg K, respectively, under a magnetic field of 1.5 T. In general, it was verified that the magnetic entropy change achieved for La0.7Ca0.3Mn1 - xNixO3 manganites synthesized via the auto-combustion method is higher than those reported for other manganites with comparable Ni2+-doping levels synthesized via standard solid state reaction. The addition of Ni2+ increases the value of the relative cooling power as compared to that of the parent compound. The highest value of this parameter (∼60 J/kg) is found for a Ni-doping level of 2% around 230 K in a field of 1.5 T.

  9. Magnetic and magnetocaloric properties of Gd(Ni1-xFex)2 quasi-binary Laves phases with x = 0.04 ÷ 0.16

    Science.gov (United States)

    Anikin, Maksim; Tarasov, Evgeniy; Kudrevatykh, Nikolay; Inishev, Aleksander; Semkin, Mikhail; Volegov, Aleksey; Zinin, Aleksander

    2018-03-01

    In this paper the results of specific magnetization (M), heat capacity (Cp) and magnetocaloric effect (MCE) measurements for Gd(Ni1-xFex)2 system over the Ni substitution by Fe range of x = 0 ÷ 0.16 are presented. Phase composition was controlled by X-ray diffraction analysis. Heat capacity was measured in the temperature range 77 ÷ 320 K. MCE has been studied within the temperature range 5 ÷ 400 K in magnetic fields up to 70 kOe by the entropy magnetic contribution change calculation (ΔSm) and by direct ΔTad measurements at the adiabatic conditions for external magnetic field change ΔH = ±17.5 kOe. It was found that the Fe concentration increase causes both the Cp maxima disappearing at Curie temperature point and emergence of magnetic contribution to Cp in a wide temperature range below this point. Moreover, in compounds with iron, a plateau-like temperature dependence of the MCE was observed for both magnetic entropy change (ΔSm) and direct ΔTad data which are independent on Fe concentration. The possible reasons of such behavior are discussed.

  10. Magnetic and magnetocaloric properties in second-order phase transition La1-xKxMnO3 and their composites

    Science.gov (United States)

    Thanh, Tran Dang; Linh, Dinh Chi; Yen, Pham Duc Huyen; Bau, Le Viet; Ky, Vu Hong; Wang, Zhihao; Piao, Hong-Guang; An, Nguyen Manh; Yu, Seong-Cho

    2018-03-01

    In this work, we present a detailed study on the magnetic properties and the magnetocaloric effect (MCE) of La1-xKxMnO3 compounds with x=0.05-0.2. Our results pointed out that the Curie temperature (TC) could be controlled easily from 213 to 306 K by increasing K-doping concentration (x) from 0.05 to 0.2. In the paramagnetic region, the inverse of the susceptibility can be analyzed by using the Curie-Weiss law, χ(T)=C/(T-θ). The results have proved an existence of ferromagnetic clusters at temperatures above TC. Based on Banerjee's criteria, we also pointed out that the samples are the second-order phase transition materials. Their magnetic entropy change was calculated by using the Maxwell relation and a phenomenological model. Interestingly, the samples with x=0.1-0.2 exhibit a large MCE in a range of 282-306 K, which are suitable for room-temperature magnetic refrigeration applications. The composites obtained from single phase samples (x=0.1-0.2) exhibit the high relative cooling power values in a wide temperature range. From the viewpoint of the refrigerant capacity, the composites formed out of La1-xKxMnO3 will become more useful for magnetic refrigeration applications around room-temperature.

  11. Magnetic and magnetocaloric properties of perovskite manganite Pr0.55Sr0.45MnO3

    International Nuclear Information System (INIS)

    Fan Jiyu; Pi Li; Zhang Lei; Tong Wei; Ling Langsheng; Hong Bo; Shi Yangguang; Zhang Weichun; Lu Di; Zhang Yuheng

    2011-01-01

    In this paper, we have studied the magnetic and magnetocaloric properties of the perovskite manganite Pr 0.55 Sr 0.45 MnO 3 . It shows a sharp paramagnetic-ferromagnetic phase transition at 291 K and possesses a moderate magnetic entropy change near room temperature. In addition, a large relative cooling power (143.64 J/kg) and a wide temperature range (84 K) have been found in this material. Compare with the Landau model, we find that the itinerant electrons mainly contribute the larger magnetic entropy change at paramagnetic region.

  12. Magnetocaloric refrigeration concepts: current state of the art

    DEFF Research Database (Denmark)

    Nielsen, Kaspar Kirstein

    2014-01-01

    of designs and concepts. In this paper key parts constituting a magnetocaloric refrigeration device are reviewed in terms of how they have been implemented in actual machines. Some of the major design choices are then evaluated and, based on numerical modeling tools, recommendations on how to optimize...

  13. Giant barocaloric effect in hexagonal Ni2In-type Mn-Co-Ge-In compounds around room temperature

    Science.gov (United States)

    Wu, Rong-Rong; Bao, Li-Fu; Hu, Feng-Xia; Wu, Hui; Huang, Qing-Zhen; Wang, Jing; Dong, Xiao-Li; Li, Guan-Nan; Sun, Ji-Rong; Shen, Fei-Ran; Zhao, Tong-Yun; Zheng, Xin-Qi; Wang, Li-Chen; Liu, Yao; Zuo, Wen-Liang; Zhao, Ying-Ying; Zhang, Ming; Wang, Xian-Cheng; Jin, Chang-Qing; Rao, Guang-Hui; Han, Xiu-Feng; Shen, Bao-Gen

    2015-12-01

    The most widespread cooling techniques based on gas compression/expansion encounter environmental problems. Thus, tremendous effort has been dedicated to develop alternative cooling technique and search for solid state materials that show large caloric effects. An application of pressure to a material can cause a change in temperature, which is called the barocaloric effect. Here we report the giant barocaloric effect in a hexagonal Ni2In-type MnCoGe0.99In0.01 compound involving magnetostructural transformation, Tmstr, which is accompanied with a big difference in the internal energy due to a great negative lattice expansion(ΔV/V ~ 3.9%). High resolution neutron diffraction experiments reveal that the hydrostatic pressure can push the Tmstr to a lower temperature at a rate of 7.7 K/kbar, resulting in a giant barocaloric effect. The entropy change under a moderate pressure of 3 kbar reaches 52 Jkg-1K-1, which exceeds that of most materials, including the reported giant magnetocaloric effect driven by 5 T magnetic field that is available only by superconducting magnets.

  14. Direct measurements of the magnetocaloric effect

    DEFF Research Database (Denmark)

    Nielsen, Kaspar Kirstein; Bahl, Christian R.H.; Neves Bez, Henrique

    2014-01-01

    We present an experimental setup recently developed at DTU Energy Conversion for measuring specific heat and direct isothermal entropy change in a varying magnetic field (DSC device) using calorimetry. The device operates in high vacuum (~1e-6 mbar) and measurements are fully automated with respect...

  15. Magnetocaloric effect across the coupled structural and ...

    Indian Academy of Sciences (India)

    Wintec

    Sande P, Hueso L E, Miguens D R, Rivas J,. Rivadulla F and Lopez Quintela M A 2001 Appl. Phys. Lett. 79 2040. 13. Pecharsky V K, Gschneidner Jr K A and Tsokol A O. 2005 Rep. Prog. Phys. 68 1479. 14. Sheng-Bo Tian, Manh-Huong Phan, Seong-Cho Yu and Nam Hwi Hur 2003 Physica B327 221. 15. de Oliveira N A ...

  16. Studies on magnetocaloric and magnetic coupling effects =

    Science.gov (United States)

    Amaral, Joao Cunha de Sequeira

    O presente trabalho apresenta novas metodologias desenvolvidas para a analise das propriedades magneticas e magnetocaloricas de materiais, sustentadas em consideracoes teoricas a partir de modelos, nomeadamente a teoria de transicoes de fase de Landau, o modelo de campo medio molecular e a teoria de fenomeno critico. Sao propostos novos metodos de escala, permitindo a interpretacao de dados de magnetizacao de materiais numa perspectiva de campo medio molecular ou teoria de fenomeno critico. E apresentado um metodo de estimar a magnetizacao espontanea de um material ferromagnetico a partir de relacoes entropia/magnetizacao estabelecidas pelo modelo de campo medio molecular. A termodinamica das transicoes de fase magneticas de primeira ordem e estudada usando a teoria de Landau e de campo medio molecular (modelo de Bean-Rodbell), avaliando os efeitos de fenomenos fora de equilibrio e de condicoes de mistura de fase em estimativas do efeito magnetocalorico a partir de medidas magneticas. Efeitos de desordem, interpretados como uma distribuicao na interaccao magnetica entre ioes, estabelecem os efeitos de distribuicoes quimicas/estruturais nas propriedades magneticas e magnetocaloricas de materiais com transicoes de fase de segunda e de primeira ordem. O uso das metodologias apresentadas na interpretacao das propriedades magneticas de variados materiais ferromagneticos permitiu obter: 1) uma analise quantitativa da variacao de spin por iao Gadolinio devido a transicao estrutural do composto Gd5Si2Ge2, 2) a descricao da configuracao de cluster magnetico de ioes Mn na fase ferromagnetica em manganites da familia La-Sr e La-Ca, 3) a determinacao dos expoentes criticos β e δ do Niquel por metodos de escala, 4) a descricao do efeito da pressao nas propriedades magneticas e magnetocaloricas do composto LaFe11.5Si1.5 atraves do modelo de Bean-Rodbell, 5) uma estimativa da desordem em manganites ferromagneticas com transicoes de segunda e primeira ordem, 6) uma descricao de campo medio das propriedades magneticas da liga Fe23Cu77, 7) o estudo de efeitos de separacao de fase na familia de compostos La0.70-xErxSr0.30MnO3 e 8) a determinacao realista da variacao de entropia magnetica na familia de compostos de efeito magnetocalorico colossal Mn1-x-yFexCryAs.

  17. Materials for Room Temperature Magnetic Refrigeration

    DEFF Research Database (Denmark)

    Hansen, Britt Rosendahl

    to change its temperature when a magnetic field is applied or removed. For room temperature cooling, one utilizes that the magnetocaloric effect peaks near magnetic phase transitions and so the materials of interest all have a critical temperature within the range of 250 – 310 K. A magnetic refrigerant...... should fulfill a number of criteria, among these a large magnetic entropy change, a large adiabatic temperature change, preferably little to no thermal or magnetic hysteresis and the material should have the stability required for long term use. As the temperature range required for room temperature......Magnetic refrigeration is a cooling method, which holds the promise of being cleaner and more efficient than conventional vapor-compression cooling. Much research has been done during the last two decades on various magnetic materials for this purpose and today a number of materials are considered...

  18. A concise approach for building the s-T diagram for Mn-Fe-P-Si hysteretic magnetocaloric material

    Science.gov (United States)

    Christiaanse, T. V.; Campbell, O.; Trevizoli, P. V.; Misra, S.; van Asten, D.; Zhang, L.; Govindappa, P.; Niknia, I.; Teyber, R.; Rowe, A.

    2017-09-01

    The use of first order magnetocaloric materials (FOM’s) in magnetic cycles is of interest for the development of efficient magnetic heat pumps. FOM’s present promising magnetocaloric properties; however, hysteresis reduces the reversible adiabatic temperature change (Δ Tad ) of these materials, and consequently, impacts performance. The present paper evaluates the reversible Δ Tad in a FOM. Six samples of the Mn-Fe-P-Si material with different transition temperatures are examined. The samples are measured for heat capacity, magnetization, and adiabatic temperature change using heating and cooling protocols to characterize hysteresis. After correcting demagnetizing fields, the entropy-temperature (s-T ) diagrams are constructed and used to calculate adiabatic temperature change using four different thermal paths. The post-calculated Δ Tad is compared with experimental data from direct Δ Tad measurements. Most of the samples of Mn-Fe-P-Si show that post-calculated Δ Tad resulting from the heating zero field and cooling in-field entropy curves align best with the Δ Tad measurements. The impact of the demagnetizing field is shown in terms of absolute variation to the post-calculated Δ Tad . A functional representation is used to explain observed data sensitivities in the post-calculated Δ Tad .

  19. Tuning the magnetocaloric response in half-Heusler/Heusler MnNi1 +xSb solid solutions

    Science.gov (United States)

    Levin, Emily E.; Bocarsly, Joshua D.; Wyckoff, Kira E.; Pollock, Tresa M.; Seshadri, Ram

    2017-12-01

    Materials with a large magnetocaloric response are associated with a temperature change upon the application of a magnetic field and are of interest for applications in magnetic refrigeration and thermomagnetic power generation. The usual metric of this response is the gravimetric isothermal entropy change Δ SM . The use of a simple proxy for the Δ SM that is based on density functional theory (DFT) calculations of the magnetic electronic structure suggests that half-Heusler MnNiSb should be a better magnetocaloric than the corresponding Heusler compound MnNi2Sb . Guided by this observation, we present a study of MnNi1 +xSb (x =0 , 0.25, 0.5, 0.75, and 1.0) to evaluate relevant structural and magnetic properties. DFT stability calculations suggest that the addition of Ni takes place at a symmetrically distinct Ni site in the half-Heusler structure and support the observation using synchrotron x-ray diffraction of a homogeneous solid solution between the half-Heusler and Heusler end members. There is a maximum in the saturation magnetization at x =0.5 and the Curie temperature systematically decreases with increasing x . Δ SM for a maximum magnetic field change of Δ H =5 T monotonically decreases in magnitude from -2.93 J kg-1K-1 in the half-Heusler to -1.35 J kg-1K-1 in the Heusler compound. The concurrent broadening of the magnetic transition results in a maximum in the refrigerant capacity at x =0.75 . The Curie temperature of this system is highly tunable between 350 K and 750 K, making it ideal for low grade waste heat recovery via thermomagnetic power generation. The increase in Δ SM with decreasing x may be extendable to other MnNi2Z Heusler systems that are currently under investigation for use in magnetocaloric refrigeration applications.

  20. Quantifying Temperature Effects on Fall Chinook Salmon

    Energy Technology Data Exchange (ETDEWEB)

    Jager, Yetta [ORNL

    2011-11-01

    The motivation for this study was to recommend relationships for use in a model of San Joaquin fall Chinook salmon. This report reviews literature pertaining to relationships between water temperature and fall Chinook salmon. The report is organized into three sections that deal with temperature effects on development and timing of freshwater life stages, temperature effects on incubation survival for eggs and alevin, and temperature effects on juvenile survival. Recommendations are made for modeling temperature influences for all three life stages.

  1. Observation of low temperature metastable states in complex CaMn7O12

    Science.gov (United States)

    Jain, Parul; Bansal, Dipanshu; Sharma, Gyaneshwar; Bhattacharya, Anupam; Ingale, Babita; Delaire, Olivier; Chatterjee, Ratnamala

    2018-02-01

    The low temperature magnetic behaviour of the multiferroic quadruple perovskite CaMn7O12 is investigated. The magneto-caloric effect in this material is presented for the first time. Along with the established magnetic transitions, T N1 ~ 90 K and T N2 ~ 45 K, an anomaly at 20 K is observed in our dc magnetization, ac susceptibility and dielectric measurements; below which, an inverse magnetocaloric effect is also observed in our  ‑ΔS M (T) plots. The neutron scattering measurements show minimal change between 10 K and 30 K in static correlations, but a clear change in energy and linewidth of the magnetic excitations is evident. The results suggest that only dynamic correlations change across T M ~ 20 K. The existence of multiple magnetic interactions below 45 K, with significant coupling between them, is demonstrated using an Arrott plot analysis of our magnetic data. Compatible conclusions are drawn from magnetocaloric plots. The peak change in isothermal magnetic entropy (‑ΔS M) is 1.3 JK‑1 kg‑1 and the value of refrigeration capacity in CaMn7O12 is 34.5 J · kg‑1 at 7 T.

  2. Structural, magnetic and magnetocaloric properties of La{sub 0.7}Ca{sub 0.2}Sr{sub 0.1}Mn{sub 1−x}Cr{sub x}O{sub 3} compounds with x = 0, 0.05 and 0.1

    Energy Technology Data Exchange (ETDEWEB)

    Dhahri, Ah., E-mail: dhahri.ahmad@outlook.fr [Laboratoire de Physique Appliquée, Faculté des Sciences de Sfax, BP 1171, Université de Sfax, 3000 (Tunisia); Jemmali, M. [Laboratoire des Sciences des Matériaux et de l’Environnement, Faculté des Sciences de Sfax, BP 1171, Université de Sfax, 3000 (Tunisia); Taibi, K. [Département SDM, FGMGP/USTHB, 16311 (Algeria); Dhahri, E. [Laboratoire de Physique Appliquée, Faculté des Sciences de Sfax, BP 1171, Université de Sfax, 3000 (Tunisia); Hlil, E.K. [Institut Néel, CNRS et Université J. Fourier, BP 166, 38042 Grenoble (France)

    2015-01-05

    Highlights: • The samples crystallize in the rhombohedral structure with the R3{sup ¯}c space group. • Enhancement of T{sub C} for the rhombohedral samples. • The relative cooling power increases with Cr-doping. • All samples exhibit a large magnetocaloric effect. • High values of the magnetoresistance in all samples. - Abstract: Structural, magnetic and magnetocaloric properties of La{sub 0.7}Sr{sub 0.1}Ca{sub 0.2}Mn{sub 1−x}Cr{sub x}O{sub 3} compounds with x = 0, 0.05 and 0.1 have been investigated to shed light on Cr-doping influence. X-ray diffraction studies show that all samples crystallize in the rhombohedral symmetry with R3{sup ¯}c space group. Rietveld refinement structure shows that the insertion of Cr in Mn network modifies the structural parameters such as the volume, Mn–O–Mn angles and the Mn–O bond length. The substitution of Mn by Cr decreases the 2p-3d hybridization between O and Mn ions, reduces the bandwidth and increases the electron–phonon coupling. The investigation of magnetic and magnetocaloric properties reveals that the samples exhibit a paramagnetic(PM)–ferromagnetic (FM) transition with decreasing Curie temperature (T{sub C}) from 294 K to 255 K when Cr doping level increases. The magnetic entropy change (ΔS{sub M}{sup max}) also decreases from 6.20 J kg{sup −1} K{sup −1} for x = 0 to3.80 J kg{sup −1} K{sup −1} for x = 0.1, while the relative cooling power (RCP) increases from 234.5 to 240 J kg{sup −1}, respectively, under a magnetic field of 5 T. These outcomes suggest that Mn-site Cr doping inhibits the enhancement of the magnetocaloric effect in some perovskite manganites. This is explained by the weakening of the ferromagnetic double-exchange interaction between Mn{sup 3+} and Mn{sup 4+} ions.

  3. A large magnetic entropy change near room temperature in La0.8Ba0.1Ca0.1Mn0.97Fe0.03O3 perovskite

    International Nuclear Information System (INIS)

    Ghodhbane, S.; Tka, E.; Dhahri, J.; Hlil, E.K.

    2014-01-01

    Highlights: • The prepared samples exhibit paramagnetic–ferromagnetic phase transition (T C ). • Arrott plots show phase transition of the second order. • Large magnetocaloric effect is reported based on the first order phase transition. • Noticeable |ΔS M | at low field makes the system useful for magnetic refrigeration. - Abstract: In this paper, we have studied the structural, magnetic and magnetocaloric properties of the perovskite manganite La 0.8 Ba 0.1 Ca 0.1 Mn 0.97 Fe 0.03 O 3 . X-ray diffraction pattern has been recorded at room temperature and this could be indexed to the rhombohedra perovskite structure with space group. The magnetocaloric effect and transition order were investigated by dc magnetization measurement. A maximum entropy change of 4.28 J/kg K and a refrigerant capacity of 241 J/kg were observed at an external field change of 5 T. The phenomenon of large magnetic entropy change and the convenient adjustment of the Curie temperature make the perovskite-type manganese oxides useful for magnetic refrigerants in an extended high temperature range even at room temperature (RT)

  4. A Magnetocaloric Pump for Lab-On-A-Chip Technology: Phase I Report

    Energy Technology Data Exchange (ETDEWEB)

    Love, LJL

    2004-05-08

    A magnetocaloric pump provides a simple means of pumping fluid using only external thermal and magnetic fields. The principle, which can be traced back to the early work of Rosensweig, is straightforward. Magnetic materials tend to lose their magnetization as the temperature approaches the material's Curie point. Exposing a column of magnetic fluid to a uniform magnetic field coincident with a temperature gradient produces a pressure gradient in the magnetic fluid. As the fluid heats up, it loses its attraction to the magnetic field and is displaced by cooler fluid. The impact of such a phenomenon is obvious: fluid propulsion with no moving mechanical parts. Until recently, limitations in the magnetic and thermal properties of conventional materials severely limited practical operating pressure gradients. However, recent advancements in the design of metal substituted magnetite enable fine control over both the magnetic and thermal properties of magnetic nanoparticles, a key element in colloidal based magnetic fluids (ferrofluids). This manuscript begins with a basic description of the process and previous limitations due to material properties. This is followed by a review of existing methods of synthesizing magnetic nanoparticles as well as an introduction to a new approach based on thermophilic metal-reducing bacteria. We compare two compounds and show, experimentally, significant variation in specific magnetic and thermal properties. We develop the constitutive thermal, magnetic, and fluid dynamic equations associated with magnetocaloric pump and validate our finite element model with a series of experiments. Preliminary results show a good match between the model and experiment as well as approximately an order of magnitude increase in the fluid flow rate over conventional magnetite based ferrofluids operating below 80 C. Finally, as a practical demonstration, we describe a novel application of this technology: pumping fluids at the &apos

  5. A Magnetocaloric Pump for Lab-On-Chip Technology: Phase I Report

    Energy Technology Data Exchange (ETDEWEB)

    Love, L.J.

    2004-04-05

    A magnetocaloric pump provides a simple means of pumping fluid using only external thermal and magnetic fields. The principle, which can be traced back to the early work of Rosensweig, is straightforward. Magnetic materials tend to lose their magnetization as the temperature approaches the material's Curie point. Exposing a column of magnetic fluid to a uniform magnetic field coincident with a temperature gradient produces a pressure gradient in the magnetic fluid. As the fluid heats up, it loses its attraction to the magnetic field and is displaced by cooler fluid. The impact of such a phenomenon is obvious: fluid propulsion with no moving mechanical parts. Until recently, limitations in the magnetic and thermal properties of conventional materials severely limited practical operating pressure gradients. However, recent advancements in the design of metal substituted magnetite enable fine control over both the magnetic and thermal properties of magnetic nanoparticles, a key element in colloidal based magnetic fluids (ferrofluids). This manuscript begins with a basic description of the process and previous limitations due to material properties. This is followed by a review of existing methods of synthesizing magnetic nanoparticles as well as an introduction to a new approach based on thermophilic metal-reducing bacteria. We compare two compounds and show, experimentally, significant variation in specific magnetic and thermal properties. We develop the constitutive thermal, magnetic, and fluid dynamic equations associated with magnetocaloric pump and validate our finite element model with a series of experiments. Preliminary results show a good match between the model and experiment as well as approximately an order of magnitude increase in the fluid flow rate over conventional magnetite based ferrofluids operating below 80 C. Finally, as a practical demonstration, we describe a novel application of this technology: pumping fluids at the &apos

  6. EFFECTS OF ELEVATED TEMPERATURE ON ELEVATED ...

    African Journals Online (AJOL)

    eobe

    concrete. Data obtained at 7 and 28 days for the effects of temperature with compressive strength are shown in Tables 1 and 2 respectively while the loss of weight as related to elevated temperature and age, are in. Figure 1. The effect of elevated temperature on the compressive strength at 7 days and 28 days for concrete ...

  7. Investigation of the magnetic, electronic and magnetocaloric properties of La0.7(Ca,Sr)0.3Mn1-xGdxO3 manganites

    Science.gov (United States)

    Riahi, K.; Ezaami, A.; Messaoui, I.; Solzi, M.; Cheikhrouhou-Koubaa, W.; Cugini, F.; Allodi, G.; Rossi, F.; Cheikhrouhou, A.

    2017-11-01

    La0.7(Ca,Sr)0.3Mn1-xGdxO3 (with x = 0; x = 2% and x = 6%) manganites samples have been studied by several techniques including X-ray diffraction (XRD), Scanning Electron Microscopy (SEM), 55Mn and 139La nuclear magnetic resonance (NMR) spectroscopy and magnetometric measurements. The X-ray powder diffraction shows that all the prepared samples are single phase. La0.7Ca0.15Sr0.15MnO3 manganite is crystallized in the rhombohedral structure, whereas a structural transition towards orthorhombic system is observed for x ≥ 2%. Magnetization as a function of temperature shows that all samples exhibit a ferromagnetic (FM)-paramagnetic (PM) phase transition. Gadolinium doping in Manganese site was found to induce a strong initial decrease of the Curie temperature TC. The single double-exchange-narowed 55Mn NMR line, though broadened by Gd, demonstrates a metallic state in all samples. The current manganites exhibit a second-order magnetic phase transition at TC, which is also confirmed by the criterion of Banerjee. In addition, the normalized entropy change curves of all the compounds collapse onto a universal master curve, a further signature of a second-order transition. The Gd-doped compounds undergo a large magnetocaloric effect, with an enhanced width TFWHM of the entropy change peak as compared to the Gd-free materials, and have consequently potential applications in magnetic refrigeration.

  8. The influence of disorder on magnetocaloric effect and the order of transition in ferromagnetic manganite (La{sub 1-x}Nd{sub x}){sub 2/3}(Ca{sub 1-y}Sr{sub y}){sub 1/3}MnO{sub 3}

    Energy Technology Data Exchange (ETDEWEB)

    Khelifi, J. [Universite de Sfax, Laboratoire de Physique Appliquee, Faculte des Sciences de Sfax, Sfax (Tunisia); CNRS et Universite Joseph Fourier, Institut Neel, Grenoble (France); Tozri, A.; Dhahri, E. [Universite de Sfax, Laboratoire de Physique Appliquee, Faculte des Sciences de Sfax, Sfax (Tunisia)

    2014-09-15

    Magnetocaloric effect and order of transition in (La{sub 1-x}Nd{sub x}){sub 2/3}(Ca{sub 1-y}Sr{sub y}){sub 1/3}MnO{sub 3}, prepared by conventional solid-state reaction, have been investigated. Using Banerjee criterion, we demonstrate first-order transition for (J1) and (J2) as well as second-order transition for (J3), (J4), and (J5) samples. The ΔS{sub M}{sup max} is ranging between 9.18 Jkg{sup -1} K{sup -1} and 4.87 when Nd and Sr content changes leading to relative cooling power (RCP) varying between 330 and 229.35 J/kg. Both ΔS{sub M}{sup max} and the RCP are found sensitive to the disorder σ{sup 2}. The universal behavior obtained from ΔS variation curves confirmed the first-order transition for (J1) and (J2) samples and second-order transition for (J3), (J4), and (J5) samples obtained by Banerjee criterion. All samples with second-order phase transition exhibit inhomogeneous character estimated from local exponent n. (orig.)

  9. Magnetic and magnetocaloric study of manganite compounds Pr{sub 0.5}A{sub 0.05}Sr{sub 0.45}MnO{sub 3} (A=Na and K) and composite

    Energy Technology Data Exchange (ETDEWEB)

    Jerbi, A.; Krichene, A. [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, B. P. 1171, 3000 Sfax (Tunisia); Chniba-Boudjada, N. [Institut NEEL, B.P. 166, 38042 Grenoble Cedex 9 France (France); Boujelben, W., E-mail: Wahibaboujelben@yahoo.fr [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, B. P. 1171, 3000 Sfax (Tunisia)

    2015-11-15

    Structural, magnetic and magnetocaloric properties of Pr{sub 0.5}A{sub 0.05}Sr{sub 0.45}MnO{sub 3} (A=Na and K) have been investigated. Our samples have been elaborated by the conventional ceramic method at high temperature. X-ray diffraction patterns using Rietveld refinement reveal that our compounds are single phase and crystallize in the orthorhombic structure with Pbnm space group. Magnetization measurements versus temperature under an applied magnetic field of 50 mT indicate that all our investigated samples exhibit a paramagnetic–ferromagnetic transition with decreasing temperature. The values of the Curie temperatures are 270 K and 275 K for A=Na and K, respectively. The magnetocaloric study of a manganite-based composite reveals an enhancement of relative cooling power which is around 67.37% of pure Gd under an applied magnetic field of 5 T.

  10. Tunable magnetostructural coupling and large magnetocaloric effect in Mn{sub 1−x}Ni{sub 1−x}Fe{sub 2x}Si{sub 1−x}Ga{sub x}

    Energy Technology Data Exchange (ETDEWEB)

    Zhang, C.L., E-mail: zhangcl@jiangnan.edu.cn [School of Science, Jiangnan University, WuXi 214122 (China); Nie, Y.G.; Shi, H.F.; Ye, E.J.; Zhao, J.Q. [School of Science, Jiangnan University, WuXi 214122 (China); Han, Z.D. [Jiangsu Laboratory of Advanced Functional Materials, Department of Physics, Changshu Institute of Technology, Changshu 215500 (China); Xuan, H.C. [College of Materials Science and Engineering, Taiyuan University of Technology, Taiyuan 030024 (China); Wang, D.H. [National Laboratory of Solid State Microstructures, Department of Physics, Nanjing University, Nanjing 210093 (China)

    2017-06-15

    Highlights: • Realizing FM/PM-type magnetostructural transition by co-substitution at both three atomic sites of MnNiSi. • Magnetostructural transition temperature is tunable in a broad temperature window of 285 K spanning room temperature. • Relatively high M{sub S} for the orthorhombic phase and large ΔM across the magnetostructural transition. • Relatively large magnetic entropy changes and broad working temperature span. - Abstract: A common method of realizing a magnetostructural coupling for MnNiSi is chemically alloying it with a ternary compound possessing a stable Ni{sub 2}In-type structure. In this way, the substituting elements and levels are determined by the stoichiometry of counterpart compounds. In this work, chemical co-substitutions of Fe and Ga at three different atomic sites of MnNiSi were performed. The selections of substitution elements and levels were based on the site occupation rule and an analysis of the site-dependent substitutional effects on structural stability, Curie temperatures, and magnetic moment of MnNiSi. A broad Curie temperatures window of 285 K spanning room temperature was established in Mn{sub 1−x}Ni{sub 1−x}Fe{sub 2x}Si{sub 1−x}Ga{sub x}. Strong magnetostructural transformations with large magnetization difference were realized in this window. A relatively large magnetic entropy change of −38.1 J/kg K was observed for a field change of 5 T near room temperature in the alloy with x = 0.15.

  11. Pressure-induced three-dimensional ferromagnetic correlations in the giant magnetocaloric compound Gd.sub.5./sub.Ge.sub.4./sub..

    Czech Academy of Sciences Publication Activity Database

    Magen, C.; Arnold, Zdeněk; Morellon, L.; Skorokhod, Yuriy; Algarabel, P. A.; Ibarra, M. R.; Kamarád, Jiří

    2003-01-01

    Roč. 91, č. 20 (2003), s. 207202-1 - 207202-4 ISSN 0031-9007 R&D Projects: GA ČR GA106/02/0943 Grant - others:CICYT(ES) MAT2000-1756 Institutional research plan: CEZ:AV0Z1010914 Keywords : magneto-caloric compounds * pressure effect * magnetism Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 7.035, year: 2003

  12. Magnetic and magnetocaloric properties of itinerant-electron system Hf.sub.1-x./sub.Ta.sub.x./sub.Fe.sub.2./sub. (x = 0.125 and 0.175)

    Czech Academy of Sciences Publication Activity Database

    Diop, L.V.B.; Kaštil, Jiří; Isnard, O.; Arnold, Zdeněk; Kamarád, Jiří

    2015-01-01

    Roč. 627, Apr (2015), s. 446-450 ISSN 0925-8388 R&D Projects: GA ČR GAP204/12/0692 Institutional support: RVO:68378271 Keywords : itinerant-electron compounds * magnetic properties * magnetocaloric effect Subject RIV: BM - Solid Matter Physics ; Magnetism Impact factor: 3.014, year: 2015

  13. Study of magnetic, structural and magnetocaloric properties of La.sub.0.6./sub.Pr.sub.0.4./sub.Mn.sub.2./sub.Si.sub.2./sub. under high pressures and magnetic field

    Czech Academy of Sciences Publication Activity Database

    Kaštil, Jiří; Arnold, Zdeněk; Isnard, O.; Skourski, Y.; Kamarád, Jiří; Itié, J.P.

    2017-01-01

    Roč. 424, Feb (2017), s. 416-420 ISSN 0304-8853 R&D Projects: GA ČR GA15-03777S Institutional support: RVO:68378271 Keywords : magnetization * compressibility * magnetocaloric effect * high pressure Subject RIV: BM - Solid Matter Physics ; Magnetism OBOR OECD: Condensed matter physics (including formerly solid state physics, supercond.) Impact factor: 2.630, year: 2016

  14. Thermal stability and magnetocaloric properties of GdDyAlCo bulk metallic glasses

    Energy Technology Data Exchange (ETDEWEB)

    Liang, L. [State Key Laboratory for Advanced Metals and Materials, University of Science and Technology Beijing, Beijing 100083 (China); Hui, X. [State Key Laboratory for Advanced Metals and Materials, University of Science and Technology Beijing, Beijing 100083 (China)], E-mail: huixd01@hotmail.com; Chen, G.L. [State Key Laboratory for Advanced Metals and Materials, University of Science and Technology Beijing, Beijing 100083 (China)

    2008-01-25

    Gd{sub 56-x}Dy{sub x}Al{sub 24}Co{sub 20} (x = 16, 20 and 22) bulk metallic glasses (BMGs) alloys with a diameter of 2, 3 and 3 mm, respectively, were prepared by using copper mold casting. These alloys exhibit higher values of the glass transition temperature, crystallization temperature, and activation energy of the glass transition and crystallization, compared with those of other known rare-earth-based BMGs. A maximum magnetic entropy changes of 15.78 J/(kg K) is obtained in Gd{sub 40}Dy{sub 16}Al{sub 24}Co{sub 20}, which is the maximal among all the bulk metallic glasses, and is much larger than those of the known crystalline magnetic refrigerant compound Gd{sub 5}Si{sub 2}Ge{sub 1.9}Fe{sub 0.1} and pure Gd metal. All the three BMG alloys have a broader temperature range of the entropy change peak, resulting in larger refrigerate capacities (RC) than those of conventional crystalline materials. The excellent magnetocaloric properties combining with high thermal stability make them an attractive candidate for magnetic refrigerants in the temperature range of 20-100 K.

  15. Effects of partial Mn-substitution on magnetic and magnetocaloric properties in Pr{sub 0.7}Ca{sub 0.3}Mn{sub 0.95}X{sub 0.05}O{sub 3} (Cr, Ni, Co and Fe) manganites

    Energy Technology Data Exchange (ETDEWEB)

    Selmi, A. [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, Sfax University, B.P. 1171, 3000 Sfax (Tunisia); M’nassri, R., E-mail: rafik_mnassri@yahoo.fr [Higher Institute of Applied Sciences and Technology of Kasserine, Kairouan University, B.P. 471, 1200 Kasserine (Tunisia); Cheikhrouhou-Koubaa, W. [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, Sfax University, B.P. 1171, 3000 Sfax (Tunisia); Chniba Boudjada, N. [Institut NEEL, B.P. 166, 38042 Grenoble Cedex 9 (France); Cheikhrouhou, A. [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, Sfax University, B.P. 1171, 3000 Sfax (Tunisia)

    2015-01-15

    Highlights: • Pr{sub 0.7}Ca{sub 0.3}Mn{sub 0.95}X{sub 0.05}O{sub 3}(X = Cr, Ni, Co and Fe) ceramics were prepared by solid state method. • The manganite phases crystallize in an orthorhombic (Pnma) structure. • The samples exhibit a second order paramagnetic (PM)–ferromagnetic (FM) phase transition at the Curie temperature T{sub C}. • Maximum RCP equal to 405 J/kg observed for Pr{sub 0.7}Ca{sub 0.3}Mn{sub 0.95}Cr{sub 0.05}O{sub 3}. • Second order phase transition is confirmed by Arrott plots and universal curves of entropy change. • The experimental ΔS{sub M} are well predicted by the phenomenological universal curve. - Abstract: Structural, magnetic and magnetocaloric properties of Pr{sub 0.7}Ca{sub 0.3}Mn{sub 0.95}X{sub 0.05}O{sub 3}(X = Cr, Ni, Co and Fe) ceramics have been investigated by X-ray diffraction (XRD) and magnetic measurements. Powder samples have been elaborated using the solid state reaction method at high temperature. The Rietveld analysis of the powder X-ray diffraction shows that the samples crystallize in the orthorhombic structure with Pnma space group. Magnetic measurements show that all our materials exhibit a paramagnetic–ferromagnetic transition with decreasing temperature. The Arrott plots of ours materials reveal the occurrence of a second-order phase transition. The maximum values of magnetic entropy change |ΔS{sub M}{sup max}| are 2.92, 2.96, 3.1, and 2.38 J kg{sup −1} K{sup −1} and the relative cooling power (RCP) values are 405.8, 378.2, 352.2 and 337.4 J kg{sup −1} for a magnetic-field change from 0 to 5 T for Cr, Ni, Co and Fe respectively. The large RCP found in our substituted samples will be interesting for magnetic refrigeration over a wide temperature range ∼130 K around its paramagnetic to ferromagnetic transition temperature. With the scaling laws of ΔS{sub M}, the experimental ΔS{sub M} collapse onto a universal curve for several ceramics, where an average curve is obtained. With the

  16. Effective fuel temperature of WWER-1000

    Directory of Open Access Journals (Sweden)

    Kudrov Alexander

    2017-01-01

    Full Text Available The main temperature characteristics of a pressurized water reactor are distinguished, supporting its safety and reliable operation. The special role of the uranium fuel effective temperature is emphasized and the accuracy of the analytical determination of the power effect is increased. The calculation of the temperature distribution along the radius of the fuel rod was carried out taking into account the temperature dependence of the thermal conductivity UO2. The design procedure was corrected for using the Finca-Ronchi dependence for the thermal conductivity of 95% density of the theoretical one.

  17. Effective fuel temperature of wwer-1000

    Directory of Open Access Journals (Sweden)

    Kudrov Alexander

    2017-01-01

    Full Text Available The main temperature characteristics of a pressurized water reactor are distinguished, supporting its safety and reliable operation. The special role of the uranium fuel effective temperature is emphasized and the accuracy of the analytical determination of the power effect is increased. The calculation of the temperature distribution along the radius of the fuel rod was carried out taking into account the temperature dependence of the thermal conductivity UO2. The design procedure was corrected for using the Finca-Ronchi dependence for the thermal conductivity of 95% density of the theoretical one.

  18. Electrical and morphological properties of magnetocaloric nano ZnNi ferrite

    Science.gov (United States)

    Hemeda, O. M.; Mostafa, Nasser Y.; Abd Elkader, Omar H.; Hemeda, D. M.; Tawfik, A.; Mostafa, M.

    2015-11-01

    A series of Zn1-xNixFe2O4 nano ferrite (with x=0, 0.2, 0.4, 0.6, 0.8, and 1) compositions were synthesized using the combustion technique. The powder samples were characterized by XRD. The X-ray analysis showed that the samples were single phase spinel cubic structure. The AC resistivity decreases by increasing the frequency from 1 kHz to 10 kHz. As the frequency of the applied field increases the hopping of charge carrier also increase, thereby decreasing the resistivity. A shift in dielectric maximum is observed toward higher temperature with increasing the Ni content from 536 K to 560 K at 1 kHz. The HRTEM (high resolution TEM) images of four compositions have lattice spacing which confirms the crystalline nature of the samples. The surface morphology SEM of the sample consists of some grains with relatively homogenies distribution with an average size varying from 0.85 to 0.92 μm. The values for entropy change in this work are still small but are significally higher than the values that have been reported for iron oxide nanoparticle. The magnetic entropy change was calculated from measurements of M (H, T) where H is the magnetic field and T is the temperature. The maximum value of entropy change (ΔS) obtained near Curie temperature which makes these material candidates for magnetocaloric applications.

  19. Structural, magnetic and magnetocaloric properties of La{sub 0.8}Ca{sub 0.2−x}Na{sub x}MnO{sub 3} manganites (0≤x≤0.2)

    Energy Technology Data Exchange (ETDEWEB)

    Choura Maatar, S. [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, Sfax University, B.P. 1171, 3000 Sfax (Tunisia); M’nassri, R. [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, Sfax University, B.P. 1171, 3000 Sfax (Tunisia); Institut NEEL, CNRS, B.P.166, 38042 Grenoble Cedex 9 (France); Cheikhrouhou Koubaa, W., E-mail: wissem.koubaa@yahoo.fr [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, Sfax University, B.P. 1171, 3000 Sfax (Tunisia); Koubaa, M. [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, Sfax University, B.P. 1171, 3000 Sfax (Tunisia); Cheikhrouhou, A. [Laboratoire de Physique des Matériaux, Faculté des Sciences de Sfax, Sfax University, B.P. 1171, 3000 Sfax (Tunisia); Centre de Recherche en Informatique, Multimédia et Traitement Numérique des Données, Technopole de Sfax, Cité El Ons, Route de Tunis, Km 9, Sfax. B.P. 275, Sakiet Ezzit, 3021 Sfax (Tunisia)

    2015-05-15

    In this work, we report the effect of Na doping on the structural, magnetic and magnetocaloric properties in La{sub 0.8}Ca{sub 0.2−x}Na{sub x}MnO{sub 3} powder samples. Our polycristalline samples have been synthesized using the solid-state reaction method at high temperatures. The parent compound La{sub 0.8}Ca{sub 0.2}MnO{sub 3} crystallizes in the orthorhombic system with Pbnm space group. Na doping induces a structural transition from orthorhombic (Pbnm space group) to rhombohedral (R-3C space group) symmetry. Magnetization measurements versus temperature in a magnetic applied field of 50 mT showed that all our investigated samples display a paramagnetic-ferromagnetic transition with decreasing temperature. The Curie temperature T{sub C} increases with Na content from 240 K for x=0 to 330 K for x=0.2. A large magnetocaloric effect has been observed in all samples, the maximum entropy change, |∆S{sub M}|{sub max}, shifts to smaller values with increasing Na content, from4.56 J/kg K (x=0.05) to 2.3 J/kg K (x=0.2) under a magnetic field change ∆µ{sub 0}H of 2 T. For the same applied magnetic field of 2 T, the Relative Cooling Power (RCP) values are found to be constant around 91 J/kg. - Graphical abstract: Sodium doping induces an increase of T{sub C} from 240 K for x=0 to 330 K for x=0.2. - Highlights: • La{sub 0.8}Ca{sub 0.2−x}Na{sub x}MnO{sub 3} are synthesized using the ceramic method at high temperatures. • Na doping induces a structural transition from Pbnm to R-3C space group. • T{sub C} increases with Na content from 240 K for x=0 to 330 K for x=0.2. • RCP is constant around 91 J/kg for all compounds under 2 T.

  20. Effect of ambient pressure on Leidenfrost temperature.

    Science.gov (United States)

    Orejon, Daniel; Sefiane, Khellil; Takata, Yasuyuki

    2014-11-01

    The accurate prediction and control of the interaction of liquids with hot surfaces is paramount in numerous areas, including cooling applications. We present results illustrating the effect of ambient pressure on the temperature required for a droplet to levitate over a hot surface, i.e., the Leidenfrost temperature. In the present study the dependence of wetting and levitating temperatures on ambient pressure in a range of subatmospheric pressures is reported. Experimental data indicate that the Leidenfrost temperature decreases with decreasing pressure at subatmospheric pressures. A physical approach for the dependence of Leidenfrost temperature on ambient pressure, based on an analogy with saturation pressure dependence, is proposed. Furthermore, previous literature data for pressures above atmospheric are also included in the analysis to support and validate the proposed approach. In addition, the effect of substrate material, substrate roughness, and type of fluid on the Leidenfrost temperature is discussed.

  1. Effect of Cd doping on magnetocaloric effect and critical behavior analysis on perovskite Nd1-xCdxMnO3 (x = 0, 0.1, 0.2, 0.3, and 0.4) manganite polycrystals

    Science.gov (United States)

    Saravanan, C.; Thiyagarajan, R.; Manikandan, K.; Sathiskumar, M.; Kanjariya, P. V.; Bhalodia, J. A.; Arumugam, S.

    2017-12-01

    We report the doping effect of divalent cation Cd2+ at Nd-site of intermediate bandwidth manganite system NdMnO3 through the temperature- and magnetic field-dependent magnetization measurements. The parent compound shows paramagnetic-antiferromagnetic transition at 56 K, whereas Cd doped samples show the paramagnetic-ferromagnetic transition with fluctuating TC. During this transition, Nd1-xCdxMnO3 (x = 0.1 and 0.2) samples exhibit first order nature, whereas Nd1-xCdxMnO3 (x = 0.3 and 0.4) samples exhibit second order nature. It confirms a crossover from first order transition to second order transition while x = 0.2 to x = 0.3. By having first order transition, x = 0.2 sample exhibits high magnetic entropy change of 3.62 J kg-1 K-1 for the magnetic field change of 5 T out of all compositions. By having second order transitions, x = 0.4 sample exhibits a high relative cooling power of 319.71 J kg-1 for the magnetic field change of 5 T out of all the compositions. The critical behavior of second order transition of x = 0.3 and 0.4 samples has been analyzed using Arrott and Kouvel-Fisher plots. The estimated critical exponents of these samples are nearly matched with the mean free model, which can be explained by the existence of dipole-dipole interaction by the Cd doping which strengthens long range ferromagnetic interactions between the spins.

  2. Thermodynamics of the Heat-Flux Avalanches at the First-Order Magnetic Transition in Magnetocaloric Materials

    Science.gov (United States)

    Piazzi, Marco; Bennati, Cecilia; Basso, Vittorio

    2017-10-01

    We investigate the kinetics of first-order magnetic phase transitions by measuring and modeling the heat-flux avalanches corresponding to the irreversible motion of the phase-boundary interface separating the coexisting low- and high-temperature stable magnetic phases. By means of out-of-equilibrium thermodynamics, we encompass the damping mechanisms of the boundary motion in a phenomenological parameter αs. By analyzing the time behavior of the heat-flux signals measured on La (Fe -Mn -Si )13-H magnetocaloric compounds through Peltier calorimetry temperature scans performed at low rates, we relate the linear rise of the individual avalanches to the intrinsic-damping parameter αs.

  3. ELEVATED TEMPERATURE EFFECTS ON THE ELECTRICAL ...

    African Journals Online (AJOL)

    The effects of elevated temperatures on the electrical properties of Bi metal probe to Si thin films had been investigated for electric field values 10-100V/m. Measurements of current (I) – voltage (V) characteristics were obtained at temperatures 300,320,340,360,380 and 400K respectively. The results indicated linear I–V ...

  4. Nanoscale temperature sensing using the Seebeck effect

    NARCIS (Netherlands)

    Bakker, F. L.; Flipse, J.; van Wees, B. J.

    2012-01-01

    We experimentally study the effect of Joule heating on the electron temperature in metallic nanoscale devices and compare the results with a diffusive 3D finite element model. The temperature is probed using four thermocouples located at different distances from the heater. A good quantitative

  5. Structural, magnetic, magnetocaloric effect and critical behavior of La{sub 0.7}Sr{sub 0.3−x}□{sub x}MnO{sub 3}(0 ≤ x ≤ 0.05)

    Energy Technology Data Exchange (ETDEWEB)

    Makni-Chakroun, J., E-mail: makni.jihed@yahoo.fr [LT2S Lab, Digital Research Centre of Sfax, Sfax Technopark, BP 275, 3021 Sakiet-Ezzit (Tunisia); Sfifir, I.; Cheikhrouhou-Koubaa, W.; Koubaa, M. [LT2S Lab, Digital Research Centre of Sfax, Sfax Technopark, BP 275, 3021 Sakiet-Ezzit (Tunisia); Cheikhrouhou, A. [Material Physics Laboratory, Faculty of Sciences of Sfax, B.P. 1171, Sfax University, 3000 Sfax (Tunisia)

    2017-06-15

    Highlights: • The samples crystallize in the rhombohedral structure with R-3C space group. • Curie temperature T{sub C} decreases with lacuna. • (1/χ) versus temperature indicates Griffiths phase occurrence. • Result show that the paramagnetic-ferromagnetic transition is of second order. • Widom scaling relation confirms the critical exponent value. - Abstract: In this paper, we present the effect of Strontium vacancies on the structure and magnetic properties of La{sub 0.7}Sr{sub 0.3−x}□{sub x}MnO{sub 3} nano-sized compounds (x = 0; 0.01; 0.03 and 0.05), synthesized using the sol-gel method. X-ray diffraction revealed that these manganites crystallized in the rhombohedral structure with space group R3-C. From magnetization measurements as function of temperature and magnetic applied field, we have noticed a large magnetic entropy change (∆S{sub M}) around Curie temperature. ∆S{sub M} is found to decrease with the deficiency content (2.30 J/kg·K for x = 0–1.33 J/kg·K for x = 0.05 under magnetic field change µ{sub 0}∆H = 5 T). This behavior is accompanied by a slight reduction of the Curie temperature (T{sub C} = 338 and 328 K for x = 0 and 0.05, respectively). These results show that our materials are potential candidates for magnetic refrigerants working in above room temperature. The refined values of the critical exponents β, γ and δ obtained from the modified Arrott plots and Kouvel-Fisher method indicated that the behavior of the parent sample and the samples with 1and 3% of strontium-deficient are characterized by long-range mean-field behavior (with β = 0.50; γ = 1). However, for 5% lacuna, the magnetic behavior is close to the theoretical 3D-Heisemberg prediction with short-range exchange coupling.

  6. Universal behavior of magnetocaloric effect in a layered perovskite La{sub 1.2}Sr{sub 1.8}Mn{sub 2}O{sub 7} single crystal

    Energy Technology Data Exchange (ETDEWEB)

    Thanh, Tran Dang, E-mail: thanhxraylab@yahoo.com [Institute of Materials Science, Vietnam Academy of Science and Technology, 18-Hoang Quoc Viet, Hanoi (Viet Nam); Manh, T.V.; Ho, T.A. [Department of Physics, Chungbuk National University, Cheongju 361-763 (Korea, Republic of); Telegin, Andrey [Department of Magnetic Semiconductors, Institute of Metal Physics, RAS (Russian Federation); Phan, T.L. [Department of Physics and Oxide Research Center, Hankuk University of Foreign Studies, Yongin 449-791 (Korea, Republic of); Yu, S.C., E-mail: scyu@chungbuk.ac.kr [Department of Physics, Chungbuk National University, Cheongju 361-763 (Korea, Republic of)

    2016-04-01

    In this paper, we present a detailed analysis on temperature and magnetic field dependences of the magnetic entropy change (ΔS{sub m}) near the ferromagnetic (FM)–paramagnetic (PM) phase transition of a La{sub 1.2}Sr{sub 1.8}Mn{sub 2}O{sub 7} single crystal. Experimental results reveal the material exhibiting a FM–PM phase transition at T{sub C}=85 K, and belongs to a second-order phase transition (SOPT). Around T{sub C}, −ΔS{sub m} reaches the maximum value (|ΔS{sub max}|), which increases with increasing an applied magnetic field change, ΔH. The |ΔS{sub max}| values found are about 0.93, 1.73, 2.38, 2.91, and 3.33 J kg{sup −1} K{sup −1} for ΔH=10, 20, 30, 40, and 50 kOe, respectively. However, the peak position of the −ΔS{sub m}(T) curves is effectively shifted to higher temperatures when ΔH increases. Additionally, the ΔS{sub m}(T) curves measured at different ΔH values do not collapse into a universal curve when they are normalized to their respective ΔS{sub max} value, and Prod. Type: rescaled the temperature axis with θ{sub 1}=(T−T{sub C})/(T{sub r}−T{sub C}) for a reference temperature T{sub r}>T{sub C} or T{sub r}temperature range if using two separated reference temperatures, T{sub r1} and T{sub r2}, with θ{sub 2}=−(T−T{sub C})/(T{sub r1}−T{sub C}) for T≤T{sub C} and θ{sub 2}=(T−T{sub C})/(T{sub r2}−T{sub C}) for T>T{sub C}.

  7. MOSFET dosimetry: temperature effects in-vivo

    International Nuclear Information System (INIS)

    Yu, P.K.N.; Cheung, T.; Butson, M.J.; Cancer Services, Wollongong, NSW

    2004-01-01

    Full text: This note investigates temperature effects on dosimetry using a Metal Oxide Semiconductor Field Effect Transistor (MOSFET) for radiotherapy x-ray treatment. This was performed by analysing the dose response and threshold voltage outputs for MOSFET dosimeters as a function of ambient temperature. Results have shown the clinical semiconductor dosimetry system (CSDS) MOSFET provides stable dose measurements with temperatures varying from 15 deg C up to 40 deg C. Thus standard irradiations performed at room temperature can be directly compared to in-vivo dose assessments performed at near body temperature without a temperature correction function. The MOSFET dosimeter threshold voltage varies with temperature and this level is dependant on the dose history of the MOSFET dosimeter. However the variation can be accounted for in the measurement method. For accurate dosimetry the detector should be placed for approximately 60 seconds on a patient to allow thermal equilibrium before measurements are taken with the final reading performed whilst still attached to the patient or conversely left for approximately 120 seconds after removal from the patient if initial readout was measured at room temperature to allow temperature equilibrium to be established. Copyright (2004) Australasian College of Physical Scientists and Engineers in Medicine

  8. Effects of temperature variation on MOSFET dosimetry

    International Nuclear Information System (INIS)

    Cheung Tsang; Butson, Martin J; Yu, Peter K N

    2004-01-01

    This note investigates temperature effects on dosimetry using a metal oxide semiconductor field effect transistor (MOSFET) for radiotherapy x-ray treatment. This was performed by analysing the dose response and threshold voltage outputs for MOSFET dosimeters as a function of ambient temperature. Results have shown that the clinical semiconductor dosimetry system (CSDS) MOSFET provides stable dose measurements with temperatures varying from 15 deg. C up to 40 deg. C. Thus standard irradiations performed at room temperature can be directly compared to in vivo dose assessments performed at near body temperature without a temperature correction function. The MOSFET dosimeter threshold voltage varies with temperature and this level is dependent on the dose history of the MOSFET dosimeter. However, the variation can be accounted for in the measurement method. For accurate dosimetry, the detector should be placed for approximately 60 s on a patient to allow thermal equilibrium before measurements are taken with the final reading performed whilst still attached to the patient or conversely left for approximately 120 s after removal from the patient if initial readout was measured at room temperature to allow temperature equilibrium to be established. (note)

  9. Variable effects of temperature on insect herbivory

    Directory of Open Access Journals (Sweden)

    Nathan P. Lemoine

    2014-05-01

    Full Text Available Rising temperatures can influence the top-down control of plant biomass by increasing herbivore metabolic demands. Unfortunately, we know relatively little about the effects of temperature on herbivory rates for most insect herbivores in a given community. Evolutionary history, adaptation to local environments, and dietary factors may lead to variable thermal response curves across different species. Here we characterized the effect of temperature on herbivory rates for 21 herbivore-plant pairs, encompassing 14 herbivore and 12 plant species. We show that overall consumption rates increase with temperature between 20 and 30 °C but do not increase further with increasing temperature. However, there is substantial variation in thermal responses among individual herbivore-plant pairs at the highest temperatures. Over one third of the herbivore-plant pairs showed declining consumption rates at high temperatures, while an approximately equal number showed increasing consumption rates. Such variation existed even within herbivore species, as some species exhibited idiosyncratic thermal response curves on different host plants. Thus, rising temperatures, particularly with respect to climate change, may have highly variable effects on plant-herbivore interactions and, ultimately, top-down control of plant biomass.

  10. Structural, transport, magnetic, magnetocaloric properties and critical analysis of Ni-Co-Mn-Ga Heusler alloys

    Science.gov (United States)

    Arumugam, S.; Devarajan, U.; Esakki Muthu, S.; Singh, Sanjay; Thiyagarajan, R.; Raja, M. Manivel; Rama Rao, N. V.; Banerjee, Alok

    2017-11-01

    In this work, we have investigated structural, transport, magnetic, magnetocaloric (MC) properties and critical exponents analysis of the (Ni2.1-xCox)Mn0.9 Ga (x = 0, 0.04, 0.12 and 0.2) Heusler alloys. For all compositions, cubic austenite (A) phase with metallic character is observed at room temperature (RT). With increasing of Co content, magnitude of resistivity decreases, whereas residual resistivity (ρ0) and electron scattering factor (A) increases linearly. Magnetic measurements exhibit that ferromagnetic (FM) Curie temperature (TCA) increases towards RT by increasing Co concentration. All samples show conventional MC and maximum magnetic entropy change (ΔSMpeak) of -2.8 Jkg-1 K-1 is observed for x = 0.12 at 147 K under 5 T. Further, hysteresis is observed between cooling and warming cycles around FM-PM (TCA) transition in x = 0, 0.04 samples, which suggests that first order nature of transition. However, there is no hysteresis across TCA for x = 0.12 and 0.2 samples suggesting second-order nature of the transition. The critical exponents are calculated for x = 0.12 sample around TCA using Arrott plot and Kouvel-Fisher method, the estimated critical exponents are found closer to the mean-field model reveals the long range ferromagnetic ordering in this composition.

  11. The effect of temperature in high temperature SHPB test

    International Nuclear Information System (INIS)

    Park, Kyoung Joon; Yang, Hyun Mo; Min, Oak Key

    2001-01-01

    The split Hopkinson pressure bar has used for a high strain rate impact test. Also, it has been developed and modified for compression, shear, tension, elevated temperature and subzero tests. In this paper, SHPB compression tests have been performed with pure titanium at elevated temperatures. The range of temperature is from room temperature to 1000 deg. C with interval of 200 .deg. C. To raise temperature of the specimen, a radiant heater which is composed of a pair of ellipsoidal cavities and halogen lamps is developed at high temperature SHPB test. There are some difficulties in a high temperature test such as temperature gradient, lubrication and prevention of oxidation of specimen. The temperature gradient of specimen is affected by the variation of temperature. Barreling occurred at not properly lubricated specimen. Stress-strain relations of pure titanium have been obtained in the range of strain rate at 1900/sec∼2000/sec and temperature at 25 .deg. C∼1000 .deg. C

  12. Experimental investigation of the effect of thermal hysteresis in first order material MnFe(P,As) applied in an AMR device

    DEFF Research Database (Denmark)

    von Moos, Lars; Nielsen, Kaspar Kirstein; Engelbrecht, Kurt

    2014-01-01

    The magnetocaloric first order material MnFe(P,As) is a candidate for room temperature magnetic refrigeration. However, these materials have intrinsic hysteresis and the impact on the refrigeration performance has not yet been thoroughly investigated in the literature.Here, the magnetocaloric eff...

  13. Electrical and morphological properties of magnetocaloric nano ZnNi ferrite

    Energy Technology Data Exchange (ETDEWEB)

    Hemeda, O.M., E-mail: omhemeda@yahoo.co.uk [Physics Department, Faculty of Science, Tanta University, Tanta (Egypt); Mostafa, Nasser Y. [Materials and Corrosion Group, Department of Chemistry, Faculty of Science, Taif University (Saudi Arabia); Chemistry Department, Faculty of Science, Suez Canal University, Ismailia 41522 (Egypt); Abd Elkader, Omar H. [Electron Microscope & Thin Films Department, Physics Division, National Research Center, Dokki 12622, Cairo (Egypt); Electron Microscope Unit, Zoology Department, College of Science, King Saud University, Riyadh (Saudi Arabia); Hemeda, D.M.; Tawfik, A.; Mostafa, M. [Physics Department, Faculty of Science, Tanta University, Tanta (Egypt)

    2015-11-15

    A series of Zn{sub 1–x}Ni{sub x}Fe{sub 2}O{sub 4} nano ferrite (with x=0, 0.2, 0.4, 0.6, 0.8, and 1) compositions were synthesized using the combustion technique. The powder samples were characterized by XRD. The X-ray analysis showed that the samples were single phase spinel cubic structure. The AC resistivity decreases by increasing the frequency from 1 kHz to 10 kHz. As the frequency of the applied field increases the hopping of charge carrier also increase, thereby decreasing the resistivity. A shift in dielectric maximum is observed toward higher temperature with increasing the Ni content from 536 K to 560 K at 1 kHz. The HRTEM (high resolution TEM) images of four compositions have lattice spacing which confirms the crystalline nature of the samples. The surface morphology SEM of the sample consists of some grains with relatively homogenies distribution with an average size varying from 0.85 to 0.92 μm. The values for entropy change in this work are still small but are significally higher than the values that have been reported for iron oxide nanoparticle. The magnetic entropy change was calculated from measurements of M (H, T) where H is the magnetic field and T is the temperature. The maximum value of entropy change (∆S) obtained near Curie temperature which makes these material candidates for magnetocaloric applications. - Highlights: • Nanoparticles of Ni–Zn ferrite were prepared by solution combustion method. • A shift in dielectric maximum is observed toward high temperature with increasing the Ni content. • The inter planner distance obtained from HRTEM coincide with the f XRD results. • The entropy change vs. temperature shows a broad maximum near Curie temperature. • This results are useful for the operation of cooling devices.

  14. Magnetocaloric materials and first order phase transitions

    DEFF Research Database (Denmark)

    Neves Bez, Henrique

    of the properties of such materials.The experimental characterization of these materials is done through various different methods, such as X-ray diffraction, magnetometry, calorimetry, direct measurements of entropy change, capacitance dilatometry, scanning electron microscopy,energy-dispersive X-ray spectrometry...... shows a paradoxical behavior; the material shows features of both a first order phase transition and of a second order one. Identities as shift of the heat capacity peak and an asymmetric growth of of the entropy change with magnetic field would describe this material transition as a first order one...... temperature and field independent is exaggerated and perhaps cannot be taken.A series of La(Fe,Mn,Si)13Hz with slightly changes in the composition is also evaluated here. This material may present a second order phase transition for large content of Mn and Si, which will become a first order one as the Mn...

  15. Effects of Temperature on Hybrid Lens Performance

    Science.gov (United States)

    Askins, Steve; Victoria, Marta; Herrero, Rebeca; Domínguez, César; Antón, Ignacio; Sala, Gabriel

    2011-12-01

    In hybrid Silicone-on-glass Fresnel lenses, an optical silicone is molded onto a glass substrate and forms the Fresnel structure. These lenses offer a cost effective solution as a primary optical element in point-focus concentrator photovoltaic modules, as well as performance advantages. However, these lenses have a high performance variation with temperature due both to the change in index of refraction of silicone as well as to deformations in the facets caused by coefficient of thermal expansion (CTE) mismatch. In this study we perform measurements of the light flux at the focal plane of a family of SOG lenses, varying temperature and lens-to-receiver distances. The effect of varying silicone cure temperature and the depth of the silicone between the lens and the glass substrate on temperature dependence was investigated. A preliminary computer model of this behavior is presented.

  16. Effects of temperature increase in insect community

    International Nuclear Information System (INIS)

    Tuda, Midori; Fujii, Koichi

    1993-01-01

    Temperature will rise by 2degC in the near future. Potential effects of the rise on biological community are predicted with little evidence on the subjects. Individualistic responses of component species in community are often ignored. We performed experiments on a lab host-parasitoid community and tested the hypothesis that individualistic changes in developmental schedules by temperature rise can generate drastic community change. (author)

  17. Effects of temperature increase in insect community

    Energy Technology Data Exchange (ETDEWEB)

    Tuda, Midori; Fujii, Koichi (Tsukuba Univ., Ibaraki (Japan))

    1993-01-01

    Temperature will rise by 2degC in the near future. Potential effects of the rise on biological community are predicted with little evidence on the subjects. Individualistic responses of component species in community are often ignored. We performed experiments on a lab host-parasitoid community and tested the hypothesis that individualistic changes in developmental schedules by temperature rise can generate drastic community change. (author).

  18. Effect of temperature on quantum dots

    Indian Academy of Sciences (India)

    MAHDI AHMADI BORJI

    2017-07-12

    Jul 12, 2017 ... Abstract. In this paper, the strain, band-edge, and energy levels of pyramidal InxGa1−xAs/GaAs quantum dots are investigated by 1-band effective mass approach. It is shown that while temperature has no remarkable effect on the strain tensor, the band gap lowers and the radiation wavelength elongates ...

  19. Temperature effects on cathodoluminescence of enstatite

    Science.gov (United States)

    Ohgo, S.; Nishido, H.

    2017-12-01

    Cathodoluminescence (CL) of enstatite has been extensively investigated for planetary science applications. The CL features are affected by many factors of impurities such as transition metal elements, structural defects and sample temperature. However, the temperature effects on enstatite CL have not been clarified so far. In this study, we have quantitatively evaluated temperature effects on enstatite CL. Three samples of luminescent enstatite were employed for CL spectral measurements. Color CL imaging was carried out using a cold-cathode type Luminoscope with a cooled-CCD camera. CL spectroscopy was made by a SEM-CL system, which is comprised of SEM (JEOL: JSM-5410LV) combined with a grating monochromator (OXFORD: Mono CL2). The CL emitted from the sample was collected in the range of 300-800 nm with a photomultiplier tube by a photon counting method at various temperatures from -193-50 degree C. All CL spectra were corrected for total instrumental response. Color CL imaging reveals various CL emissions with red, reddish-purple and bluish-purple in the terrestrial and extraterrestrial enstatite. All of them have two broad emission bands at around 400 nm in a blue region and at around 670 nm in a red region at room and liquid nitrogen temperatures. The spectral peak in a red region is sharpened and enhanced at lower temperature due to reduction of thermal lattice vibration and an increase in luminescent efficiency. CL intensity at around 670 nm of enstatite decreases with an increase in sample temperature up to -110 degree C from -193 degree C, and increases with an increase in sample temperature between -110 and 50 degree C. This behavior is not able to be explained by a temperature quenching theory based on an increase in the probability of non-radiative transition with the rise of temperature. A least-square fitting of the Arrhenius plot by assuming a Mott-Seitz model provides an activation energy of less than 0.01 eV in temperature quenching process from

  20. Effect of irrigation fluid temperature on body temperature during ...

    African Journals Online (AJOL)

    ... of dogs were hypothermic (<37oC). The addition of warmed irrigation fluids to a temperature management protocol in dogs undergoing elbow arthroscopy during general anaesthesia did not lead to decreased temperature losses. Keywords: Arthroscopy, Hypothermia, Irrigation fluid temperature, Thermoregulation.

  1. Effective Tolman temperature induced by trace anomaly

    Energy Technology Data Exchange (ETDEWEB)

    Eune, Myungseok [Sangmyung University, Department of Civil Engineering, Cheonan (Korea, Republic of); Gim, Yongwan [Sogang University, Department of Physics, Seoul (Korea, Republic of); Sogang University, Research Institute for Basic Science, Seoul (Korea, Republic of); Kim, Wontae [Sogang University, Department of Physics, Seoul (Korea, Republic of)

    2017-04-15

    Despite the finiteness of stress tensor for a scalar field on the four-dimensional Schwarzschild black hole in the Israel-Hartle-Hawking vacuum, the Tolman temperature in thermal equilibrium is certainly divergent on the horizon due to the infinite blue-shift of the Hawking temperature. The origin of this conflict is due to the fact that the conventional Tolman temperature was based on the assumption of a traceless stress tensor, which is, however, incompatible with the presence of the trace anomaly responsible for the Hawking radiation. Here, we present an effective Tolman temperature which is compatible with the presence of the trace anomaly by using the modified Stefan-Boltzmann law. Eventually, the effective Tolman temperature turns out to be finite everywhere outside the horizon, and so an infinite blue-shift of the Hawking temperature at the event horizon does not appear any more. In particular, it is vanishing on the horizon, so that the equivalence principle is exactly recovered at the horizon. (orig.)

  2. Effective Tolman temperature induced by trace anomaly

    International Nuclear Information System (INIS)

    Eune, Myungseok; Gim, Yongwan; Kim, Wontae

    2017-01-01

    Despite the finiteness of stress tensor for a scalar field on the four-dimensional Schwarzschild black hole in the Israel-Hartle-Hawking vacuum, the Tolman temperature in thermal equilibrium is certainly divergent on the horizon due to the infinite blue-shift of the Hawking temperature. The origin of this conflict is due to the fact that the conventional Tolman temperature was based on the assumption of a traceless stress tensor, which is, however, incompatible with the presence of the trace anomaly responsible for the Hawking radiation. Here, we present an effective Tolman temperature which is compatible with the presence of the trace anomaly by using the modified Stefan-Boltzmann law. Eventually, the effective Tolman temperature turns out to be finite everywhere outside the horizon, and so an infinite blue-shift of the Hawking temperature at the event horizon does not appear any more. In particular, it is vanishing on the horizon, so that the equivalence principle is exactly recovered at the horizon. (orig.)

  3. Nuclear shell effects at high temperatures

    International Nuclear Information System (INIS)

    Davidson, N.J.; Miller, H.G.

    1993-01-01

    In discussing the disappearance of nuclear shell effects at high temperatures, it is important to distinguish between the ''smearing out'' of the single-particle spectrum with increasing temperature and the vanishing of shell related structures in many-body quantities such as the excitation energy per nucleon. We propose a semiempirical method to obtain an upper bound on the temperature required to smooth the single-particle spectrum, and point out that shell effects in many-body parameters may persist above this temperature. We find that the temperature required to smear out the single-particle spectrum is approximately 1 MeV for heavy nuclei (A approx-gt 150) and about 3--4 MeV for light nuclei (A approx-lt 50), in reasonable agreement with the estimate of 41/πA 1/3 obtained from calculations with harmonic oscillator potentials. These temperatures correspond to many-body excitation energies of approximately 20 and 60 MeV, respectively

  4. Effects of temperature changes on groundwater ecosystems

    Science.gov (United States)

    Griebler, Christian; Kellermann, Claudia; Schreglmann, Kathrin; Lueders, Tillmann; Brielmann, Heike; Schmidt, Susanne; Kuntz, David; Walker-Hertkorn, Simone

    2014-05-01

    The use of groundwater as a carrier of thermal energy is becoming more and more important as a sustainable source of heating and cooling. At the same time, the present understanding of the effects of aquifer thermal usage on geochemical and biological aquifer ecosystem functions is extremely limited. Recently we started to assess the effects of temperature changes in groundwater on the ecological integrity of aquifers. In a field study, we have monitored hydrogeochemical, microbial, and faunal parameters in groundwater of an oligotrophic aquifer in the vicinity of an active thermal discharge facility. The observed seasonal variability of abiotic and biotic parameters between wells was considerable. Yet, due to the energy-limited conditions no significant temperature impacts on bacterial or faunal abundances and on bacterial productivity were observed. In contrast, the diversity of aquifer bacterial communities and invertebrate fauna was either positively or negatively affected by temperature, respectively. In follow-up laboratory experiments temperature effects were systematically evaluated with respect to energy limitation (e.g. establishment of unlimited growth conditions), geochemistry (e.g. dynamics of DOC and nutrients), microbiology (e.g. survival of pathogens), and fauna (temperature preference and tolerance). First, with increased nutrient and organic carbon concentrations even small temperature changes revealed microbiological dynamics. Second, considerable amounts of adsorbed DOC were mobilized from sediments of different origin with an increase in temperatures. No evidence was obtained for growth of pathogenic bacteria and extended survival of viruses at elevated temperatures. Invertebrates clearly preferred natural thermal conditions (10-12°C), where their highest frequency of appearance was measured in a temperature gradient. Short-term incubations (48h) of invertebrates in temperature dose-response tests resulted in LT50 (lethal temperature) values

  5. Comparative analysis on temperature reduction effectiveness of ...

    African Journals Online (AJOL)

    Comparative analysis on temperature reduction effectiveness of ornamental tree species in University of Port Harcourt. ... The process of urbanization causes alterations in the landscape, affects the environment negatively and the community is placed at risk. In an attempt to sustain urban growth, urban areas have now ...

  6. SUPPLEMENTARY INFORMATION Temperature effects on the ...

    Indian Academy of Sciences (India)

    Windows User

    SUPPLEMENTARY INFORMATION. Temperature effects on the hydrophobic force between two graphene-like surfaces in liquid water. TUHIN SAMANTA and BIMAN BAGCHI. Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore, Karnataka 560. 012, India. Table of Contents. Figure S1. Page 2.

  7. Effect of programmed circadian temperature fluctuations on ...

    African Journals Online (AJOL)

    to our knowledge of the effects of temperature on the population dynamics of freshwater snails and its bearing on their .... 28"C regime as reflected by the net reproduction rate recorded in Table 1. It was demonstrated by De Kock & .... ANDREW ARlHA, H.G. & BIRCH, L.C. 1954. The distribution and abundance of animals.

  8. Effects of chilling temperatures on photosynthesis

    Science.gov (United States)

    Environmental stress is an inescapable reality for most plants growing in natural settings. Conditions of sub or supra-optimal temperatures, water deficit, water logging, salinity, and pollution can have dramatic effects on plant growth and development, and in agricultural settings, yield. In cotton...

  9. Anomalies of kinetic coefficients in HoS near the magnetic ordering temperature

    International Nuclear Information System (INIS)

    Novikov, V.I.; Golubkov, A.V.; Kizhaev, S.A.

    1982-01-01

    A complex experimental investigation of holmium sulfide has been carried out at 1.6-90K temperature and magnetic field intensity up to 17.3 kOe. Transfer phenomena, magnetic susceptibility, magnetocaloric effect and also peculiariries of thermal conductivity were studied. All investigations were carried out using one polycrystalline holmium monosulfide sample. Antiferromagnetic character of ordering of these compounds has been established. The special anomaly of the electric conductivity temperature dependence close to the Neel temperature of 17.5 K has been revealed. Estimation of the exchange interaction integral J(o)=0.017 eV has been carried out. Experimental data on the thermal electromotive force temperature dependence close to the Neel temperature were compared with the theory of kinetic phenomena of antiferromagnetic materials

  10. Temperature standards, what and where: resources for effective temperature measurements

    International Nuclear Information System (INIS)

    Johnston, W.W. Jr.

    1982-01-01

    Many standards have been published to describe devices, methods, and other topics. How they are developed and by whom are briefly described, and an attempt is made to extract most of those relating to temperature measurements. A directory of temperature standards and their sources is provided

  11. Temperature effect on surface oxidation of titanium

    International Nuclear Information System (INIS)

    Vaquilla, I.; Barco, J.L. del; Ferron, J.

    1990-01-01

    The effect of temperature on the first stages of the superficial oxidation of polycrystalline titanium was studied using both Auger electron spectroscopy (AES) and emission shreshold (AEAPS). The number of compounds present on the surface was determined by application of the factor analysis technique. Reaction evolution was followed through the relative variation of Auger LMM and LMV transitions which are characteristic of titanium. Also the evolution of the chemical shift was determined by AEAPS. The amount of oxygen on the surface was quantified using transition KLL of oxygen. It was found that superficial oxidation depends on temperature. As much as three different compounds were determined according to substrate temperature and our exposure ranges. (Author). 7 refs., 5 figs

  12. Crystal structure, magnetic and magnetocaloric properties of aluminum-doped La{sub 0.6}Sr{sub 0.4}MnO{sub 3} perovskites

    Energy Technology Data Exchange (ETDEWEB)

    Elhamza, Amal; Dhahri, J. [Universite de Monastir, Laboratoire de la Matiere Condensee et des Nanosciences, Monastir (Tunisia); Rhouma, F.I.H. [Centre de Recherche des Sciences et Technologies de l' Energie, Laboratoire de Photovoltaique de Semi-Conducteurs et de Nanostructures, Hammam-Lif (Tunisia); Hlil, E.K. [CNRS-Universite Joseph Fourier, Institut Neel, Grenoble (France)

    2017-05-15

    In this paper, we report on the structural, magnetic and magnetocaloric properties of a series of nanocrystallines La{sub 0.6}Sr{sub 0.4}Mn{sub 1-x}Al{sub x}O{sub 3} (0 ≤ x ≤ 0.2) which were prepared by the sol-gel method. The X-ray powder diffraction showed that all our synthesized samples were of a single phase and have crystallized in the hexagonal symmetry with R anti 3c space group. Magnetic measurements showed that the sample exhibits a ferromagnetic-to-paramagnetic phase transition at a Curie temperature close to 206 K. The maximum value of the magnetic entropy change vertical stroke ΔS{sub M}{sup max} vertical stroke was found to be 1.09 J kg{sup -1} K{sup -1} for an applied magnetic field of 5T. At this value of magnetic field, the relative cooling power was 141 J kg{sup -1}. Our result on magnetocaloric properties suggests that La{sub 0.6}Sr{sub 0.4}Mn{sub 1-x}Al{sub x}O{sub 3} nanopowder with (0 ≤ x ≤ 0.2) is attractive as a potential refrigerant for high-temperature magnetic refrigeration. (orig.)

  13. Investigation on the structural, magnetic and magnetocaloric properties of nanocrystalline Pr-deficient Pr1-xSrxMnO3-δ manganites

    Science.gov (United States)

    Arun, B.; Athira, M.; Akshay, V. R.; Sudakshina, B.; Mutta, Geeta R.; Vasundhara, M.

    2018-02-01

    We have investigated the structural, magnetic and magnetocaloric properties of nanocrystalline Pr-deficient Pr1-xSrxMnO3-δ Perovskite manganites. Rietveld refinement of the X-ray powder diffraction patterns confirms that all the studied compounds have crystallized into an orthorhombic structure with Pbnm space group. Transmission electron microscopy analysis reveals nanocrystalline compounds with crystallite size less than 50 nm. The selected area electron diffraction patterns reveal the highly crystalline nature of the compounds and energy dispersive X-ray spectroscopic analysis shows that the obtained compositions are nearly identical with the nominal one. The oxygen stoichiometry is estimated by iodometric titration method and stoichiometric compositions are confirmed by X-ray Fluorescence Spectrometry analysis. A large bifurcation is observed in the ZFC/FC curves and Arrott plots not show a linear relation but have a convex curvature nature. The temperature dependence of inverse magnetic susceptibility at higher temperature confirms the existence of ferromagnetic clusters. The experimental results reveal that the reduction of crystallite size to nano metric scale in Pr-deficient manganites adversely influences structural, magnetic and magnetocaloric properties as compared to its bulk counterparts reported earlier.

  14. Martensitic transition near room temperature and the temperature- and magnetic-field-induced multifunctional properties of Ni49CuMn34In16 alloy

    Science.gov (United States)

    Sharma, V. K.; Chattopadhyay, M. K.; Khandelwal, A.; Roy, S. B.

    2010-11-01

    A near room-temperature martensitic transition is observed in the ferromagnetic austenite state of Ni50Mn34In16 alloy with 2% Cu substitution at the Ni site. Application of magnetic field in the martensite state induces a reverse martensitic transition in this alloy. dc magnetization, magnetoresistance and strain measurements in this alloy reveal that associated with this martensitic transition there exist a large magnetocaloric effect, a large magnetoresitance and a magnetic-field temperature-induced strain. This NiMnIn alloy system thus is an example of an emerging class of magnetic materials whose physical properties can be tuned by suitable chemical substitutions, to achieve magnetic-field and temperature-induced multifunctional properties at and around room temperature

  15. Effect of Gas Turbine Exhaust Temperature, Stack Temperature and Ambient Temperature on Overall Efficiency of Combine Cycle Power Plant

    OpenAIRE

    M.N.Khan; K.P.Tyagi

    2010-01-01

    The gas turbine exhaust temperature, stack temperature and ambient temperature play a very important role during the predication of the performance of combine cycle power plant. This paper covers parametric analysis of effects of gas turbine exhaust temperature, stack temperature and ambient temperature on the overall efficiency of combine cycle power plant keeping the gas turbine efficiency as well as steam turbine efficiency constant. The results shows that out of three variables i.e. turbi...

  16. Magnetic and magnetocaloric properties in La{sub 0.7}Ca{sub 0.3−x}Na{sub x}MnO{sub 3} exhibiting first-order and second-order magnetic phase transitions

    Energy Technology Data Exchange (ETDEWEB)

    Ho, T.A. [Department of Materials Science and Engineering, Korea University, Seoul 136-713 (Korea, Republic of); Dang, N.T. [Institute of Research and Development, Duy Tan University, Da Nang (Viet Nam); Phan, The-Long [Department of Physics and Oxide Research Center, Hankuk University of Foreign Studies, Yongin 449-791 (Korea, Republic of); Yang, D.S. [Physics Division, School of Science Education, Chungbuk National University, Cheongju 361-763 (Korea, Republic of); Lee, B.W. [Department of Physics and Oxide Research Center, Hankuk University of Foreign Studies, Yongin 449-791 (Korea, Republic of); Yu, S.C., E-mail: scyu@chungbuk.ac.kr [Department of Physics, Chungbuk National University, Cheongju 361-763 (Korea, Republic of)

    2016-08-15

    Polycrystalline orthorhombic samples La{sub 0.7}Ca{sub 0.3−x}Na{sub x}MnO{sub 3} (x = 0–0.09) were prepared by solid-state reaction. The study of magnetic properties revealed that the ferromagnetic-paramagnetic (FM-PM) transition temperature (T{sub C}) increases from 255 to about 271 K with increasing Na-doping content (x) from 0 to 0.09, respectively. Around the T{sub C}, we have found the samples showing a large magnetocaloric (MC) effect with maximum values of magnetic entropy change (|ΔS{sub max}|) of 7–8 J kg{sup −1} K{sup −1} and relative cooling power RCP = 232–236 J/kg for the samples x = 0.03–0.09 in a magnetic-field interval ΔH = 40 kOe. Detailed analyses of isothermal magnetization data M(T, H) based on Banerjee's criteria indicated a first-to-second-order magnetic-phase transformation taking place at a threshold Na-doping concentration x{sub c} ≈ 0.06. This could also be observed clearly from the feature of entropy universal curves. An assessment of the magnetic-ordering exponent N = dLn|ΔS{sub m}|/dLnH demonstrates an existence of short-range magnetic order in the samples. We believe that the changes of the magnetic properties and MC effect in La{sub 0.7}Ca{sub 0.3−x}Na{sub x}MnO{sub 3} caused by Na doping are related to the changes in the structural parameters and Mn{sup 4+}/Mn{sup 3+} ratio, which are confirmed by the geometrical and electronic analyses based on X-ray diffraction and X-ray absorption fine structure. - Highlights: • Geometrical and electronic structures of La{sub 0.7}Ca{sub 0.3−x}Na{sub x}MnO{sub 3}. • Threshold of first-to-second-order phase transformation in La{sub 0.7}Ca{sub 0.3−x}Na{sub x}MnO{sub 3}. • Large magneto-caloric effect with |ΔS{sub max}| ≈ 7–8 J kg{sup −1} K{sup −1}, and RCP = 232–236 J/kg. • Universal curve of magnetic-entropy change.

  17. Isotopic effect in high temperature superconductors

    International Nuclear Information System (INIS)

    Ohno, Takashi

    2000-01-01

    It is well-known that it essentially contributed to construct the BCB theory that a mechanism on formation of the Cooper pairs was dependent upon a lattice oscillation to change a critical temperature, T(sub c) of a superconductor with isotopic displacement. In this paper, here was, at first, described on an isotopic index actually measured to high temperature superconductors, and was introduced on a study on selective displacement of oxygen position. And then, a detailed measurement of 63-Cu(2) nuclear quadrupole resonance (NQR) at a plane position of YBa2Cu4O8 (Y1248) displaced with 18-O and 16-O, discussion of the isotopic effect on a base of 63-Cu(2) nuclear spin-lattice relaxation ratio, and consideration on the isotopic index according to the isotopic effect were described. As a result of the considerations, it could be concluded that the isotopic effect in a high temperature superconductor proved that antiferromagnetic spin fluctuation was an origin of Cooper pairs cohesive strength. (G.K.)

  18. Structural, magnetic and magnetocaloric properties of La{sub 0.8}Ba{sub 0.2}Mn{sub 1-x}Fe{sub x}O{sub 3} compounds with 0 Less-Than-Or-Slanted-Equal-To x Less-Than-Or-Slanted-Equal-To 0.1

    Energy Technology Data Exchange (ETDEWEB)

    Ghodhbane, S., E-mail: godhbane.sana@gmail.com [Laboratoire de la matiere condensee et des nanosciences, Departement de Physique, Faculte des Sciences, Universite de Monastir, Monastir 5019 (Tunisia); Dhahri, A.; Dhahri, N. [Laboratoire de la matiere condensee et des nanosciences, Departement de Physique, Faculte des Sciences, Universite de Monastir, Monastir 5019 (Tunisia); Hlil, E.K. [Institut Neel, CNRS-Universite J. Fourier, BP 166, 38042 Gronoble (France); Dhahri, J. [Laboratoire de la matiere condensee et des nanosciences, Departement de Physique, Faculte des Sciences, Universite de Monastir, Monastir 5019 (Tunisia)

    2013-02-15

    Highlights: Black-Right-Pointing-Pointer The prepared samples exhibit paramagnetic-ferromagnetic phase transition (T{sub C}). Black-Right-Pointing-Pointer La{sub 0.8}Ba{sub 0.2}MnO{sub 3} exhibits the highest value of 4.15 J/(K kg) for T{sub C} = 295 K. Black-Right-Pointing-Pointer The field dependence of {Delta}S{sub M} change is also analyzed showing the power law dependence. Black-Right-Pointing-Pointer Critical behavior of the transition for manganites is sensitive to the Mn-site. - Abstract: The present study reports the effect of Fe doping on the structural, magnetic and magnetocaloric proprieties in the La{sub 0.8}Ba{sub 0.2}Mn{sub 1-x}Fe{sub x}O{sub 3} (0 Less-Than-Or-Slanted-Equal-To x Less-Than-Or-Slanted-Equal-To 0.1) perovskites. The studied samples were synthesized as powder samples by solid state reaction at high temperature. Their analysis by powder X-ray diffraction using Rietveld refinement showed that they crystallize in the rhombohedral system with the R3{sup Macron }C space group. They display a paramagnetic (PM)-ferromagnetic (FM) phase transition with decreasing temperature. All of them exhibit a maximum and large magnetocaloric effect near the Curie temperature (T{sub C}). The magnitude of the isothermal magnetic entropy |{Delta}S{sub M}{sup max}| at the FM Curie temperature decreases from 4.15 J kg{sup -1} K{sup -1} for the x = 0 composition to 2.62 J kg{sup -1} K{sup -1} for x = 0.1, for a magnetic field change of 5T. For an applied magnetic field of 5T, the relative cooling power (RCP) values are found to vary between 211 and 238 J kg{sup -1}. The phenomenon of large entropy change and the convenient adjustment of the Curie temperature make these peroskite-type manganese oxides useful for magnetic refrigeration in an extended high temperature range even at room temperature.

  19. Saturation effects in Na lidar temperature measurements

    International Nuclear Information System (INIS)

    von der Gathen, P.

    1991-01-01

    Na atoms residing in the 80-110 km altitude region can be used to probe the Doppler-broadened hyperfine structure (hfs) of their D 2 resonance by ground-bases lidar and hence to deduce atmospheric temperatures. In principle, two different methods may be employed: (1) wavelength scanning of the hfs with a narrow-band laser and signal detection with a broad-band receiver, and (2) use of a broad-band laser and wavelength scanning of the hfs with a narrow-band receiver. These two methods are affected in different ways by laser-induced saturation in the Na layer, the effect on the measurements of sodium densities and of atmospheric temperatures being quite different. Density measurements are affected by the absolute level of saturation. Temperature measurements, however, are affected by the difference in saturation at the scanned wavelengths. If, additionally, observed signal levels are taken into account, method 1 is more efficient than method 2 for both types of measurements at nighttime, whereas a modified method 2 surpasses method 1 for temperature measurements at daytime

  20. Temperature dependence of the Casimir effect

    Energy Technology Data Exchange (ETDEWEB)

    Brevik, I [Department of Energy and Process Engineering, Norwegian University of Science and Technology, N-7491 Trondheim (Norway); Aarseth, J B [Department of Structural Engineering, Norwegian University of Science and Technology, N-7491 Trondheim (Norway)

    2006-05-26

    In view of the increasing accuracy of Casimir experiments, there is a need for performing accurate theoretical calculations. Using accurate experimental data for the permittivities we present, via the Lifshitz formula applied to the standard Casimir setup with two parallel plates, accurate theoretical results in the case of the metals Au, Cu and Al. Both similar and dissimilar cases are considered. Concentrating in particular on the finite temperature effect, we show how the Casimir pressure varies with separation for three different temperatures, T = {l_brace}1, 300, 350{r_brace}K. The metal surfaces are taken to be perfectly plane. The experimental data for the permittivities generally yield results that are in a good agreement with those calculated from the Drude relation with finite relaxation frequency. We give the results in a tabular form, in order to facilitate the assessment of the temperature correction which is on the 1% level. We emphasize two points: (i) the most promising route for a definite experimental verification of the finite temperature correction appears to be to concentrate on the case of large separations (optimum around 2 {mu}m); and (ii) there is no conflict between the present kind of theory and the Nernst theorem in thermodynamics.

  1. Magnetic properties and magnetocaloric response of mixed valence La{sub 2/3}Ba{sub 1/3}Mn{sub 1−x}Fe{sub x}O{sub 3} manganites

    Energy Technology Data Exchange (ETDEWEB)

    Betancourt, I., E-mail: israelb@unam.mx [Departamento de Materiales Metálicos y Cerámicos, Instituto de Investigaciones en Materiales, Universidad Nacional Autónoma de México, México D.F. 04510, México (Mexico); Lopez Maldonado, L.; Elizalde Galindo, J.T. [Instituto de Ingeniería y Tecnología, Universidad Autónoma de Ciudad Juárez, Ciudad Juárez 32310, México (Mexico)

    2016-03-01

    Polycrystalline manganites of composition La{sub 2/3}Ba{sub 1/3}Mn{sub 1−x}Fe{sub x}O{sub 3} (x=0.0–0.10) were obtained by the Pechini method. Magnetic properties exhibited a marked dependence with Fe content, showing significant reductions for the saturation magnetization and the Curie temperature. The magnetocaloric effect was quantified for all the samples by means of the magnetic entropy variations, which showed a maximum of 1.46 J/kgK for Fe content of x=0.025. Results were interpreted on the basis of a deleterious effect on the double exchange interaction provoked by the presence of Fe{sup 3+} ions within the crystal structure. - Highlights: • Polycrystalline LaBa(Mn,Fe)MnO{sub 3} manganites can be obtained by Pechini method. • Ferromagnetism can be modulated by small Fe{sup 3+} content via reduced DE interaction. • Magnetic entropy variation of −1.46 J/kgK is attainable in LaBa-based manganites.

  2. Nonequilibrium Brownian motion beyond the effective temperature.

    Directory of Open Access Journals (Sweden)

    Andrea Gnoli

    Full Text Available The condition of thermal equilibrium simplifies the theoretical treatment of fluctuations as found in the celebrated Einstein's relation between mobility and diffusivity for Brownian motion. Several recent theories relax the hypothesis of thermal equilibrium resulting in at least two main scenarios. With well separated timescales, as in aging glassy systems, equilibrium Fluctuation-Dissipation Theorem applies at each scale with its own "effective" temperature. With mixed timescales, as for example in active or granular fluids or in turbulence, temperature is no more well-defined, the dynamical nature of fluctuations fully emerges and a Generalized Fluctuation-Dissipation Theorem (GFDT applies. Here, we study experimentally the mixed timescale regime by studying fluctuations and linear response in the Brownian motion of a rotating intruder immersed in a vibro-fluidized granular medium. Increasing the packing fraction, the system is moved from a dilute single-timescale regime toward a denser multiple-timescale stage. Einstein's relation holds in the former and is violated in the latter. The violation cannot be explained in terms of effective temperatures, while the GFDT is able to impute it to the emergence of a strong coupling between the intruder and the surrounding fluid. Direct experimental measurements confirm the development of spatial correlations in the system when the density is increased.

  3. Temperature Effects on Labor in Latin America

    Science.gov (United States)

    Foreman, T.

    2016-12-01

    It has long been known that environmental conditions can affect humans' performance of various tasks, both physical and mental. In light of projected climate change, heat's impact on performance is of particular concern. While there is evidence that performance suffers, from an economic standpoint, how this performance effect changes a worker's ability or willingness to work is of particular concern. Workers' decisions to supply less labor may be a key channel for economic losses due to climate change, especially in developing countries that experience high temperatures and humidity. In a study of worker behavior in Guatemala, Mexico, and Nicaragua, increasing temperatures by 1°C was found to reduce labor supplied by up to an hour per day for each worker on average in the poorest and hottest places. This result holds across different levels of risk exposure to heat, indicating little evidence of potential adaptation measures.

  4. Effective temperature in relaxation of Coulomb glasses.

    Science.gov (United States)

    Somoza, A M; Ortuño, M; Caravaca, M; Pollak, M

    2008-08-01

    We study relaxation in two-dimensional Coulomb glasses up to macroscopic times. We use a kinetic Monte Carlo algorithm especially designed to escape efficiently from deep valleys around metastable states. We find that, during the relaxation process, the site occupancy follows a Fermi-Dirac distribution with an effective temperature much higher than the real temperature T. Long electron-hole excitations are characterized by T(eff), while short ones are thermalized at T. We argue that the density of states at the Fermi level is proportional to T(eff) and is a good thermometer to measure it. T(eff) decreases extremely slowly, roughly as the inverse of the logarithm of time, and it should affect hopping conductance in many experimental circumstances.

  5. Mo2NiB2-type Sm2Co2Al and Sm2Co2Ga compounds: Magnetic properties and giant low-temperature coercivity

    Science.gov (United States)

    Morozkin, A. V.; Garshev, A. V.; Yapaskurt, V. O.; Yao, Jinlei; Nirmala, R.; Quezado, S.; Malik, S. K.

    2018-04-01

    The magnetic ordering of Mo2NiB2-type Sm2Co2Al and Sm2Co2Ga (Immm, No. 71, oI10) compounds has been established using bulk magnetic measurements. Polycrystalline Sm2Co2Al and Sm2Co2Ga undergo ferromagnetic transitions (TC) at 50 K and 62 K, respectively, and low-temperature field induced transitions (Tm) around 14 K and 16 K (in a field of 10 kOe), respectively. Between TC and Tm Sm2Co2Al and Sm2Co2Ga are soft ferromagnets. Below Tm Sm2Co2Al and Sm2Co2Ga exhibit permanent magnet properties with a residual magnetization per samarium of 0.38 μB and 0.36 μB, respectively, and a large coercive field of 69 kOe and 72 kOe, respectively, at 5 K. The magnetocaloric effects of Sm2Co2Al and Sm2Co2Ga were calculated in terms of isothermal magnetic entropy change and they reach maximum values of -1.62 J/kg K and -1.31 J/kg K for a field change of 50 kOe at 50 K and 58 K, respectively. Low temperature magnetic ordering with enhanced anisotropy in Sm2Co2Al and Sm2Co2Ga is accompanied by a positive magnetocaloric effect with isothermal magnetic entropy changes of +1.63 J/kg K and +1.06 J/kg K for a field change of 50 kOe at 10 K and 8 K, respectively. The magnetocaloric effects of Sm2Co2Al and Sm2Co2Ga were calculated in terms of isothermal magnetic entropy change and they reach maximum values of -1.62 J/kg K and -1.31 J/kg K for a field change of 50 kOe at 50 K and 58 K, respectively. Low temperature magnetic ordering with enhanced anisotropic effects in Sm2Co2Al and Sm2Co2Ga is accompanied by a positive magnetocaloric effect with isothermal magnetic entropy changes of +1.63 J/kg K and +1.06 J/kg K for a field change of 50 kOe at 10 K and 8 K, respectively.

  6. Magnetocaloric properties of LaFe13−x−yCoxSiy and commercial grade Gd

    DEFF Research Database (Denmark)

    Bjørk, Rasmus; Bahl, Christian Robert Haffenden; Katter, M.

    2010-01-01

    The magnetocaloric properties of three samples of LaFe13−x−yCoxSiy have been measured and compared to measurements of commercial grade Gd. The samples have (x=0.86, y=1.08), (x=0.94, y=1.01) and (x=0.97, y=1.07) yielding Curie temperatures in the range 276–288 K. The magnetization, specific heat......, the specific heat capacities were 910, 840 and 835 J/kg K and the adiabatic temperature changes were 2.3, 2.1 and 2.1 K for the three LaFeCoSi samples respectively. For Gd in an internal field of 1 T the maximum specific entropy change was 3.1 J/kg K, the specific heat capacity was 340 J/kg K and the adiabatic...... temperature change was 3.3 K. The adiabatic temperature change was also calculated from the measured values of the specific heat capacity and specific magnetization and compared to the directly measured values. In general an excellent agreement was seen....

  7. Structural, magnetic, and magnetocaloric properties of bilayer manganite La1.38Sr1.62Mn2O7

    Science.gov (United States)

    Yang, Yu-E.; Xie, Yunfei; Xu, Lisha; Hu, Dazhi; Ma, Chunlan; Ling, Langsheng; Tong, Wei; Pi, Li; Zhang, Yuheng; Fan, Jiyu

    2018-04-01

    In this study, we investigated the structural, magnetic phase transition, and magnetocaloric properties of bilayer perovskite manganite La1.38Sr1.62Mn2O7 based on X-ray diffraction, electron paramagnetic resonance, and temperature-/magnetic field-dependent magnetization measurements. The structural characterization results showed the prepared sample had a tetragonal structure with the space group I4/mmm. The Curie temperature was determined as 114 K in the magnetization studies and a second-order paramagnetic-ferromagnetic transition was confirmed by the Arrott plot, which showed that the slopes were positive for all the curves. According to the variation in the electron paramagnetic resonance spectrum, we detected obvious electronic phase separation across a broad temperature range from 220 to 80 K in this magnetic material, thereby indicating that the paramagnetic and ferromagnetic phases coexist above as well as below the Curie temperature. Based on a plot of the isothermal magnetization versus the magnetic applied field, we deduced the maximum magnetic entropy change, which only reached 1.89 J/kg.K under an applied magnetic field of 7.0 T. These theoretical investigations indicated that in addition to the magnetoelastic couplings and electron interaction, electronic phase separation and anisotropic exchange interactions also affect the magnetic entropy changes in this bilayer manganite.

  8. Study of the first paramagnetic to ferromagnetic transition in as prepared samples of Mn–Fe–P–Si magnetocaloric compounds prepared by different synthesis routes

    Energy Technology Data Exchange (ETDEWEB)

    Bartok, A., E-mail: andras.bartok@satie.ens-cachan.fr [SATIE, ENS Cachan, CNRS, Universite Paris-Saclay, 61 av President Wilson, F-94230 Cachan (France); Kustov, M.; Cohen, L.F. [Imperial College, London SW7 2AZ (United Kingdom); Pasko, A. [SATIE, ENS Cachan, CNRS, Universite Paris-Saclay, 61 av President Wilson, F-94230 Cachan (France); Zehani, K.; Bessais, L. [CMTR, ICMPE, CNRS-UPEC, 2-8 rue Henri Dunant, F-94320 Thiais (France); Mazaleyrat, F.; LoBue, M. [SATIE, ENS Cachan, CNRS, Universite Paris-Saclay, 61 av President Wilson, F-94230 Cachan (France)

    2016-02-15

    Magnetocaloric materials with composition of Mn{sub 1.3}Fe{sub 0.65}P{sub 0.5} Si{sub 0.5} have been prepared by ball milling and solid-state reaction methods and consolidated using powder annealing, and conventional and spark plasma sintering. Magnetic and calorimetric measurements show remarkable differences upon first cooling, and slight differences on second and further coolings between the samples prepared by different synthesis routes. Further measurements using Hall probe imaging in high magnetic field have been also carried out. As-prepared samples have been cooled down just above the critical temperature, and the first phase transition has been induced by application of a magnetic field. Bulk samples show staircase isothermal magnetization curves whereas powders show smoother transition curves. - Highlights: • Mn–Fe–P–Si magnetocaloric materials have been prepared by different synthesis routes. • Magnetic measurements show remarkable differences upon first cooling. • First phase transition has been induced by application of a magnetic field. • Hall probe imaging in high magnetic field has also been carried out. • Bulk samples crack during the first PM–FM transition.

  9. Influence of Pb Doping on the Magnetocaloric Effect and Critical Behavior of (La0.9Dy0.1)0.8Pb0.2MnO3

    Science.gov (United States)

    Ho, T. A.; Phan, T. L.; Thang, P. D.; Yu, S. C.

    2016-05-01

    We used the modified Arrott plot method to analyze the magnetic field dependence of the magnetization, M( H), for a perovskite-type manganite (La0.9Dy0.1)0.8Pb0.2MnO3, and determined the critical parameter values T C = 248.4 K, β = 0.484 ± 0.002, γ = 0.961 ± 0.012, and δ = 2.90 ± 0.01. With these exponent values, the M( H) data around T C fall on two universal branches of a scaling function M( H, ɛ) = | ɛ| β f ±( H/| ɛ| β + γ ), where ɛ = ( T - T C)/ T C is the reduced temperature, f + for T > T C and f - for T theory (with β = 0.5, γ = 1, and δ = 3). This reveals nearly long-range ferromagnetic order existing in (La0.9Dy0.1)0.8 Pb0.2MnO3. From the M( H) data, we also found that, around the ferromagnetic-paramagnetic phase-transition temperature ( T C), the magnetic entropy change reaches a maximum value (|δ S max|) of about 1.1 J kg-1 K-1 for H = 10 kOe, corresponding to relative cooling power (RCP) of 50 J/kg. In addition to the above investigation, the temperature dependence of the magnetization, remanent magnetization ( M r), and coercivity ( H c) were recorded to learn about the physical processes taking place in (La0.9Dy0.1)0.8Pb0.2MnO3.

  10. Nonequilibrium Brownian Motion beyond the Effective Temperature

    Science.gov (United States)

    Gnoli, Andrea; Puglisi, Andrea; Sarracino, Alessandro; Vulpiani, Angelo

    2014-01-01

    The condition of thermal equilibrium simplifies the theoretical treatment of fluctuations as found in the celebrated Einstein’s relation between mobility and diffusivity for Brownian motion. Several recent theories relax the hypothesis of thermal equilibrium resulting in at least two main scenarios. With well separated timescales, as in aging glassy systems, equilibrium Fluctuation-Dissipation Theorem applies at each scale with its own “effective” temperature. With mixed timescales, as for example in active or granular fluids or in turbulence, temperature is no more well-defined, the dynamical nature of fluctuations fully emerges and a Generalized Fluctuation-Dissipation Theorem (GFDT) applies. Here, we study experimentally the mixed timescale regime by studying fluctuations and linear response in the Brownian motion of a rotating intruder immersed in a vibro-fluidized granular medium. Increasing the packing fraction, the system is moved from a dilute single-timescale regime toward a denser multiple-timescale stage. Einstein’s relation holds in the former and is violated in the latter. The violation cannot be explained in terms of effective temperatures, while the GFDT is able to impute it to the emergence of a strong coupling between the intruder and the surrounding fluid. Direct experimental measurements confirm the development of spatial correlations in the system when the density is increased. PMID:24714671

  11. Modelling and comparison studies of packed screen regenerators for active magnetocaloric refrigeration

    DEFF Research Database (Denmark)

    Lei, Tian; Engelbrecht, Kurt; Nielsen, Kaspar Kirstein

    2014-01-01

    In active magnetic regeneration (AMR) systems, not only the magnetocaloric properties of materials, but also the regenerator geometry plays an important role in the system performance. Packed sphere regenerators are often employed in existing prototypes, however, the characteristics such as relat...

  12. Modelling and comparison studies of packed screen regenerators for active magnetocaloric refrigeration

    DEFF Research Database (Denmark)

    Lei, Tian; Engelbrecht, Kurt; Nielsen, K. K.

    2011-01-01

    In active magnetic regeneration (AMR) systems, not only the magnetocaloric properties of materials, but also the regenerator geometry plays an important role in the system performance. Packed sphere regenerators are often employed in existing prototypes, however, the characteristics such as relat...

  13. Effect of microstructure on the high temperature strength of nitride

    Indian Academy of Sciences (India)

    Effect of microstructure on the high temperature strength of nitride bonded silicon carbide composite. J Rakshit P K Das. Composites Volume ... The effect of these parameters on room temperature and high temperature strength of the composite up to 1300°C in ambient condition were studied. The high temperature flexural ...

  14. Investigating the effect of surface water - groundwater interactions on stream temperature using Distributed temperature sensing and instream temperature model

    DEFF Research Database (Denmark)

    Karthikeyan, Matheswaran; Blemmer, Morten; Mortensen, Julie Flor

    2011-01-01

    Surface water–groundwater interactions at the stream interface influences, and at times controls the stream temperature, a critical water property driving biogeochemical processes. This study investigates the effects of these interactions on temperature of Stream Elverdamsåen in Denmark using...... the Distributed Temperature Sensing (DTS) system and instream temperature modelling. Locations of surface water–groundwater interactions were identified from the temperature data collected over a 2-km stream reach using a DTS system with 1-m spatial and 5-min temporal resolution. The stream under consideration...... surface water–groundwater interactions on heterogeneous behaviour of stream temperature....

  15. Investigating the effect of surface water - groundwater interactions on stream temperature using Distributed temperature sensing and instream temperature model

    DEFF Research Database (Denmark)

    Karthikeyan, Matheswaran; Blemmer, Morten; Mortensen, Julie Flor

    2011-01-01

    Surface water–groundwater interactions at the stream interface influences, and at times controls the stream temperature, a critical water property driving biogeochemical processes. This study investigates the effects of these interactions on temperature of Stream Elverdamsåen in Denmark using...... the Distributed Temperature Sensing (DTS) system and instream temperature modelling. Locations of surface water–groundwater interactions were identified from the temperature data collected over a 2-km stream reach using a DTS system with 1-m spatial and 5-min temporal resolution. The stream under consideration...... exhibits three distinct thermal regimes within a 2 km reach length due to two major interactions. An energy balance model is used to simulate the instream temperature and to quantify the effect of these interactions on the stream temperature. This research demonstrates the effect of reach level small scale...

  16. Combined scale effects for effective brazing at low temperatures

    Directory of Open Access Journals (Sweden)

    Bartout D.

    2012-12-01

    Full Text Available In modern joining technology, the focus is on effective brazing and soldering of temperature sensitive materials. Here, as well as in diffusion welding processes the needed thermal energy is externally realized in the joint zone. This produces a heating of the whole joining parts, since in laminar joining the thermal energy is transported in interior by thermal conduction. An excess of critical temperatures or tolerable impact periods in wide parts of materials and respectively components is often not avoidable. This leads to thermal damages. In this point of view nanotechnology shows promising possibilities as scale effects and their resulting thermophysical effects such as melting temperature reduction and high diffusion rates can be used for providing a self-propagating high-temperature synthesis at room temperature. After ignition by an external energy source a self-propagating exothermic reaction is started. By producing a multilayer system with alternately arranged nanoscaled layers of e.g. Al and Ni the resulting thin foil can be used as heat source for melting the braze or solder material within the joining zone without any external preheating. Due to the high process velocities up to 30 m/s and the local heat input significant thermal influences on the joined parts are not detectable.

  17. Large refrigeration capacities near room temperature in Ni{sub 2}Mn{sub 1−x}Cr{sub x}In

    Energy Technology Data Exchange (ETDEWEB)

    Brock, Jeffrey; Khan, Mahmud, E-mail: khanm2@miamioh.edu

    2017-03-01

    We report on the observation of large refrigeration capacities near room temperature in Ni{sub 2}Mn{sub 1−x}Cr{sub x}In Heusler alloys. The alloys exhibit the L2{sub 1} cubic crystal structure and undergo a second order ferromagnetic to paramagnetic phase transition. The respective Curie temperatures vary with Cr concentration from 315 K to 290 K. Net refrigerant capacities of up to 60 J/kg and 168 J/kg are observed in the alloys for applied magnetic fields of 20 kOe and 50 kOe, respectively. Due to the second order phase transition, the materials do not exhibit any hysteresis loss or other problems usually associated with materials exhibiting first order phase transitions. The observed refrigeration capacities in Ni{sub 2}Mn{sub 1−x}Cr{sub x}In are higher than those observed in many Heusler alloys with first order magnetic transitions. - Highlights: • The magnetic and magnetocaloric properties of Ni{sub 2}Mn{sub 1−x}Cr{sub x}In have been investigated. • The materials exhibit ferromagnetic transitions and associated magnetocaloric effects near room temperature. • The materials exhibit refrigeration capacities that are superior to those of Heusler alloys with first order phase transition.

  18. Magnetocaloric properties of rapidly solidified Dy{sub 3}Co alloy ribbons

    Energy Technology Data Exchange (ETDEWEB)

    Sánchez Llamazares, J. L., E-mail: jose.sanchez@ipicyt.edu.mx; Flores-Zúñiga, H.; Sánchez-Valdés, C. F. [Instituto Potosino de Investigación Científica y Tecnológica A.C., Camino a la Presa San José 2055 Col. Lomas 4" a, San Luis Potosí, S.L.P. 78216 (Mexico); Álvarez-Alonso, Pablo [Departamento de Electricidad y Electrónica, UPV/EHU, 48940 Leioa (Spain); Lara Rodríguez, G. A. [Instituto de Investigaciones en Materiales, Universidad Nacional Autónoma de México, Circuito Exterior s/n, Ciudad Universitaria, México, D. F. 04510 (Mexico); Fernández-Gubieda, M. L. [Departamento de Electricidad y Electrónica, UPV/EHU, 48940 Leioa (Spain); BC Materials, Camino de Ibaizabal, Edificio 500, Planta 1, Parque Científico y Tecnológico de Zamudio, 48160 Derio (Spain)

    2015-05-07

    The magnetic and magnetocaloric (MC) properties of melt-spun ribbons of the Dy{sub 3}Co intermetallic compound were investigated. Samples were fabricated in an Ar environment using a homemade melt spinner system at a linear speed of the rotating copper wheel of 40 ms{sup −1}. X-ray diffraction analysis shows that ribbons crystallize into a single-phase with the Fe{sub 3}C-type orthorhombic crystal structure. The M(T) curve measured at 5 mT reveals the occurrence of a transition at 32 K from a first to a second antiferromagnetic (AFM) state and an AFM-to-paramagnetic transition at T{sub N} = 43 K. Furthermore, a metamagnetic transition is observed below T{sub N}, but the magnetization change ΔM is well below the one reported for bulk alloys. Below 12 K, large inverse MC effect and hysteresis losses are observed. This behavior is related to the metamagnetic transition. For a magnetic field change of 5 T (2 T) applied along the ribbon length, the produced ribbons show a peak value of the magnetic entropy change ΔS{sub M}{sup peak} of −6.5 (− 2.1) Jkg{sup −1}K{sup −1} occurring close to T{sub N} with a full-width at half-maximum δT{sub FWHM} of 53 (37) K, and refrigerant capacity RC = 364 (83) Jkg{sup −1} (estimated from the product |ΔS{sub M}{sup peak}| × δT{sub FWHM})

  19. Effect of Temperature on Jet Velocity Spectra

    Science.gov (United States)

    Bridges, James E.; Wernet, Mark P.

    2007-01-01

    Statistical jet noise prediction codes that accurately predict spectral directivity for both cold and hot jets are highly sought both in industry and academia. Their formulation, whether based upon manipulations of the Navier-Stokes equations or upon heuristic arguments, require substantial experimental observation of jet turbulence statistics. Unfortunately, the statistics of most interest involve the space-time correlation of flow quantities, especially velocity. Until the last 10 years, all turbulence statistics were made with single-point probes, such as hotwires or laser Doppler anemometry. Particle image velocimetry (PIV) brought many new insights with its ability to measure velocity fields over large regions of jets simultaneously; however, it could not measure velocity at rates higher than a few fields per second, making it unsuitable for obtaining temporal spectra and correlations. The development of time-resolved PIV, herein called TR-PIV, has removed this limitation, enabling measurement of velocity fields at high resolution in both space and time. In this paper, ground-breaking results from the application of TR-PIV to single-flow hot jets are used to explore the impact of heat on turbulent statistics of interest to jet noise models. First, a brief summary of validation studies is reported, undertaken to show that the new technique produces the same trusted results as hotwire at cold, low-speed jets. Second, velocity spectra from cold and hot jets are compared to see the effect of heat on the spectra. It is seen that heated jets possess 10 percent more turbulence intensity compared to the unheated jets with the same velocity. The spectral shapes, when normalized using Strouhal scaling, are insensitive to temperature if the stream-wise location is normalized relative to the potential core length. Similarly, second order velocity correlations, of interest in modeling of jet noise sources, are also insensitive to temperature as well.

  20. Effects of temperature on intraspecific competition in ectotherms.

    Science.gov (United States)

    Amarasekare, Priyanga; Coutinho, Renato M

    2014-09-01

    Understanding how temperature influences population regulation through its effects on intraspecific competition is an important question for which there is currently little theory or data. Here we develop a theoretical framework for elucidating temperature effects on competition that integrates mechanistic descriptions of life-history trait responses to temperature with population models that realistically capture the variable developmental delays that characterize ectotherm life cycles. This framework yields testable comparative predictions about how intraspecific competition affects reproduction, development, and mortality under alternative hypotheses about the temperature dependence of competition. The key finding is that ectotherm population regulation in seasonal environments depends crucially on the mechanisms by which temperature affects competition. When competition is strongest at temperatures optimal for reproduction, effects of temperature and competition act antagonistically, leading to more complex dynamics than when competition is temperature independent. When the strength of competition increases with temperature past the optimal temperature for reproduction, effects of temperature and competition act synergistically, leading to dynamics qualitatively similar to those when competition is temperature independent. Paradoxically, antagonistic effects yield a higher population floor despite greater fluctuations. These findings have important implications for predicting effects of climate warming on population regulation. Synergistic effects of temperature and competition can predispose populations to stochastic extinction by lowering minimum population sizes, while antagonistic effects can increase the potential for population outbreaks through greater fluctuations in abundance.

  1. Temperature dependence of radiation effects in polyethylene

    International Nuclear Information System (INIS)

    Wu, G; Katsumura, Y.; Kudoh, H.; Morita, Y.; Seguchi, T.

    2000-01-01

    Temperature dependence of crosslinking and gas evolution under γ-irradiation was studied for high-density and low-density polyethylene samples in the 30-360degC range. It was found that crosslinking was the predominant process up to 300degC and the gel point decreased with increasing temperature. At above 300degC, however, the gel fraction at a given dose decreased rapidly with temperature and the action of radiation turned to enhance polyethylene degradation. Yields of H 2 and hydrocarbon gases increased with temperature and the compositions of hydrocarbons were dose dependent. (author)

  2. Magnetocaloric Effect and Thermoelectric Cooling - A Synergistic Cooling Technology

    Science.gov (United States)

    2018-01-16

    technologies to enable new space system capabilities. Currently, refrigeration and thermal management systems account for a large portion of the energy ... PROJECT NUMBER Robin lhnfeldt, Xia Xu , Sungho Jin, Renkun Chen, Jianlin Zheng Se. TASK NUMBER Sf. WORK UNIT NUMBER 7. PERFORMING ORGANIZATION NAME(S...SUPPLEMENTARY NOTES 14. ABSTRACT This research aims to improve efficiency of thermal management systems for space platforms. Our efforts have

  3. Magnetocaloric effect and its implementation in critical behaviour study

    Indian Academy of Sciences (India)

    From the analysis of the relationship between the local exponent n and w , other exponents β , γ and δ were calculated. Our results indicated that the ferromagnetic coupling in the La 0.67 Ca 0.33 Mn 0.9 Fe 0.1 O 3 can be well described by the 3D Heisenberg model. This reflects an existence of ferromagnetic short-range ...

  4. Magnetocaloric effect and its implementation in critical behaviour ...

    Indian Academy of Sciences (India)

    The values of maximum magnetic entropy change, full-width ... potential advantages over vapour-compression refrigeration: ..... materials obtained from the MCE scaling law method and theoretical values of three models. Composition n β γ δ. Ref. La0.67Ca0.33Mn0.9Fe0.1O3. 0.710(2). 0.418(6). 1.587(3). 4.791(3). Present.

  5. Magnetocaloric effect and its implementation in critical behaviour ...

    Indian Academy of Sciences (India)

    67Ca0.33Mn0.9Fe0.1O3. R M'NASSRI1,2. 1Higher Institute of Applied Sciences and Technology of Kasserine, Kairouan University, BP 471, 1200 Kasserine, Tunisia. 2Laboratoire de Physico-Chimie des Matériaux, Département de Physique, ...

  6. Temperature has a causal effect on avian timing of reproduction

    NARCIS (Netherlands)

    Visser, M.E.; Holleman, L.J.M.; Caro, S.P.

    2009-01-01

    Many bird species reproduce earlier in years with high spring temperatures, but little is known about the causal effect of temperature. Temperature may have a direct effect on timing of reproduction but the correlation may also be indirect, for instance via food phenology. As climate change has led

  7. Magnetic memory effects in high temperature superconductors

    International Nuclear Information System (INIS)

    Rockenbauer, A.

    1989-01-01

    Microwave absorption of high temperature oxide superconductors MBa 2 Cu 3 O 7 (M = Y, Er, Dy, Ho, Lu, Tm, Gd) at 77 K have been studied by ESR. In granular samples diamagnetic zero-field resonance and strong ESR baseline hysteresis have been observed: for increasing field sweep - a high, for decreasing one - a low, while in constant field the baseline approaches the middle position with kinetics typical of spin-glasses. The hysteresis amplitude, i.e. the deviation of high and low baselines, possesses maximum at zero field if the sample is cooled down in zero field. In case of field cooling both the diamagnetic resonance and hysteresis maximum are shifted as a function of relative direction of the fields where the samples are cooled and measured, respectively. The shift is caused by the remanent diamagnetism of trapped fluxons. The hysteresis critically depends on the modulation amplitude of magnetic field, and no hysteresis can be observed if the microwave absorption is detected without field modulation. By applying saw-tooth sweep the spin-glass can be driven between two extreme hysteresis states, and the ESR response is rectangular for large saw-tooth amplitude and linear - for small one, while for intermediate amplitudes the recording shows characteristic memory effects. The hysteresis memory is explained in terms of loop distribution of fluxons. In the single crystal the fluxon absorptions are also detected and the separation of fluxon lines can be related to the hysteresis in granular samples. (author)

  8. Effect of processor temperature on film dosimetry.

    Science.gov (United States)

    Srivastava, Shiv P; Das, Indra J

    2012-01-01

    Optical density (OD) of a radiographic film plays an important role in radiation dosimetry, which depends on various parameters, including beam energy, depth, field size, film batch, dose, dose rate, air film interface, postexposure processing time, and temperature of the processor. Most of these parameters have been studied for Kodak XV and extended dose range (EDR) films used in radiation oncology. There is very limited information on processor temperature, which is investigated in this study. Multiple XV and EDR films were exposed in the reference condition (d(max.), 10 × 10 cm(2), 100 cm) to a given dose. An automatic film processor (X-Omat 5000) was used for processing films. The temperature of the processor was adjusted manually with increasing temperature. At each temperature, a set of films was processed to evaluate OD at a given dose. For both films, OD is a linear function of processor temperature in the range of 29.4-40.6°C (85-105°F) for various dose ranges. The changes in processor temperature are directly related to the dose by a quadratic function. A simple linear equation is provided for the changes in OD vs. processor temperature, which could be used for correcting dose in radiation dosimetry when film is used. Copyright © 2012 American Association of Medical Dosimetrists. Published by Elsevier Inc. All rights reserved.

  9. Effect of processor temperature on film dosimetry

    International Nuclear Information System (INIS)

    Srivastava, Shiv P.; Das, Indra J.

    2012-01-01

    Optical density (OD) of a radiographic film plays an important role in radiation dosimetry, which depends on various parameters, including beam energy, depth, field size, film batch, dose, dose rate, air film interface, postexposure processing time, and temperature of the processor. Most of these parameters have been studied for Kodak XV and extended dose range (EDR) films used in radiation oncology. There is very limited information on processor temperature, which is investigated in this study. Multiple XV and EDR films were exposed in the reference condition (d max. , 10 × 10 cm 2 , 100 cm) to a given dose. An automatic film processor (X-Omat 5000) was used for processing films. The temperature of the processor was adjusted manually with increasing temperature. At each temperature, a set of films was processed to evaluate OD at a given dose. For both films, OD is a linear function of processor temperature in the range of 29.4–40.6°C (85–105°F) for various dose ranges. The changes in processor temperature are directly related to the dose by a quadratic function. A simple linear equation is provided for the changes in OD vs. processor temperature, which could be used for correcting dose in radiation dosimetry when film is used.

  10. Study of the first paramagnetic to ferromagnetic transition in as prepared samples of Mn-Fe-P-Si magnetocaloric compounds prepared by different synthesis routes

    Science.gov (United States)

    Bartok, A.; Kustov, M.; Cohen, L. F.; Pasko, A.; Zehani, K.; Bessais, L.; Mazaleyrat, F.; LoBue, M.

    2016-02-01

    Magnetocaloric materials with composition of Mn1.3Fe0.65P0.5 Si0.5 have been prepared by ball milling and solid-state reaction methods and consolidated using powder annealing, and conventional and spark plasma sintering. Magnetic and calorimetric measurements show remarkable differences upon first cooling, and slight differences on second and further coolings between the samples prepared by different synthesis routes. Further measurements using Hall probe imaging in high magnetic field have been also carried out. As-prepared samples have been cooled down just above the critical temperature, and the first phase transition has been induced by application of a magnetic field. Bulk samples show staircase isothermal magnetization curves whereas powders show smoother transition curves.

  11. Memory effect in the high-temperature superconducting bulks

    International Nuclear Information System (INIS)

    Zhang, Xing-Yi; Zhou, Jun; Zhou, You-He

    2013-01-01

    Highlights: •Effects of temperature cycles on levitation force relaxation are investigated. •Memory effect of the YBCO bulks is observed in experiments. •With an increase of temperature, memory of the superconductor is gradually lost. -- Abstract: We present an experimental investigation of the relaxation of vertical force components in a high-temperature superconducting levitation system with different temperature cycle processes. For a selected ambient temperature (T 1 ) of the system, the experimental results show that the relaxations of the levitation forces are strongly dependent on the initial temperature. When the sample was submitted to temperature jumps around T 1 , the sample temperature was regulated at T 2 , and there were two cases of the experiments, ΔT = T 2 − T 1 0 (positive temperature cycle). It was found that in the case of negative temperature cycle, the superconducting samples have memory effect. And for the positive temperature cycle, with the experimental temperature increase, the memory effect of samples is gradually losing. Additionally, with the increase of temperature, the influences of the negative and positive temperature cycle on the levitation force relaxation are unsymmetrical. All the results are interpreted by using the characteristics of the free energy ‘ground’ plot of the Spin-glasses qualitatively

  12. Anisotropic and excellent magnetocaloric properties of La0.7Ca0.3MnO3 single crystal with anomalous magnetization

    International Nuclear Information System (INIS)

    Debnath, J.C.; Zeng, R.; Kim, J.H.; Chen, D.P.; Dou, S.X.

    2012-01-01

    Highlights: ► ΔS M shows a very large reversibility value at low field. ► The single crystal exhibits anisotropy in the MCE. ► La 0.7 Ca 0.3 MnO 3 is weakly itinerant ferromagnetic. ► No hysteresis loss is observed. - Abstract: Magnetic properties and the magnetocaloric effect (MCE) have been investigated in La 0.7 Ca 0.3 MnO 3 single crystal with applied field along both the ab-plane and the c-direction. Due to the magnetocrystalline anisotropy, the crystal exhibits anisotropy in the MCE. Upon application of a 5 T field, the magnetic entropy changes (ΔS M ), reaching values of 7.668 J/(kg K) and 6.412 J/(kg K) for both the ab-plane and the c-direction, respectively. A magnetic entropy change of 3.3 J/(kg K) was achieved for a magnetic field change of 1.5 T at the Curie temperature, T C = 245 K. Due to the absence of grains in the single crystal, the ΔS M distribution here is much more uniform than for gadolinium (Gd) and other polycrystalline manganites, which is desirable for an Ericsson-cycle magnetic refrigerator. For a field change of 5 T, the relative cooling power, RCP, reached 358.17 J/kg, while the maximum adiabatic temperature change of 5.33 K and a magnetoresistance (MR) ratio of 507.88% at T C were observed. We analysed the magnetization of La 0.7 Ca 0.3 MnO 3 single crystal at T C and estimated several parameters of spin fluctuation on the basis of a self-consistent renormalization theory of spin fluctuations, with reciprocal susceptibility above T C . We found that the magnetic property of La 0.7 Ca 0.3 MnO 3 is weakly itinerant ferromagnetic. A large reversible MCE and no hysteresis loss with a considerable value of refrigerant capacity indicate that La 0.7 Ca 0.3 MnO 3 single crystal is a potential candidate as a magnetic refrigerant.

  13. Temperature effects on waste glass performance

    International Nuclear Information System (INIS)

    Mazer, J.J.

    1991-02-01

    The temperature dependence of glass durability, particularly that of nuclear waste glasses, is assessed by reviewing past studies. The reaction mechanism for glass dissolution in water is complex and involves multiple simultaneous reaction proceeded, including molecular water diffusion, ion exchange, surface reaction, and precipitation. These processes can change in relative importance or dominance with time or changes in temperature. The temperature dependence of each reaction process has been shown to follow an Arrhenius relationship in studies where the reaction process has been isolated, but the overall temperature dependence for nuclear waste glass reaction mechanisms is less well understood, Nuclear waste glass studies have often neglected to identify and characterize the reaction mechanism because of difficulties in performing microanalyses; thus, it is unclear if such results can be extrapolated to other temperatures or reaction times. Recent developments in analytical capabilities suggest that investigations of nuclear waste glass reactions with water can lead to better understandings of their reaction mechanisms and their temperature dependences. Until a better understanding of glass reaction mechanisms is available, caution should be exercised in using temperature as an accelerating parameter. 76 refs., 1 tab

  14. Effects of cryogenic irradiation on temperature sensors

    International Nuclear Information System (INIS)

    Courts, S.S.; Holmes, D.S.

    1996-01-01

    Several types of commercially available cryogenic temperature sensors were calibrated, irradiated at 4.2 K by a gamma or neutron source, and recalibrated in-situ to determine their suitability for thermometry in radiation environments. Comparisons were made between pre- and post-irradiation calibrations with the equivalent temperature shift calculated for each sensor at various temperature in the 4.2 K to 330 K range. Four post-irradiation calibrations were performed with annealing steps performed at 20 K, 80 K, and 330 K. Temperature sensors which were gamma irradiated were given a total dose of 10,000 Gy. Temperature sensors which were neutron irradiated were irradiated to a total fluence of 2 x 10 12 n/cm 2 . In general, for gamma radiation environments, diodes are unsuitable for use. Both carbon glass and germanium resistance sensors performed well at lower temperature, while platinum resistance sensors performed best above 30 K. Thin-film rhodium and Cernox trademark resistance sensors both performed well over the 4.2 K to 330 K range. Only thin-film rhodium and Cernox trademark resistance temperature sensors were neutron irradiated and they both performed well over the 4.2 K to 330 K range

  15. Structural, magnetic and magnetocaloric properties of Co-doped nanocrystalline La0.7Te0.3Mn0.7Co0.3O3

    Science.gov (United States)

    Meenakshi; Kumar, Amit; Mahato, Rabindra Nath

    2018-02-01

    Structural, magnetic and magnetocaloric properties of the nanocrystalline La0.7Te0.3Mn0.7Co0.3O3 perovskite manganite were investigated. X-ray diffraction pattern indicated that the nanocrystalline sample crystallized in orthorhombic crystal structure with Pbnm space group. The average particle size was calculated using scanning electron microscope and it was found to be ∼150 nm. Temperature dependence magnetization measurements revealed ferromagnetic-paramagnetic phase transition and the Curie temperature (TC) was found to be ∼201 K. Field dependence magnetization showed the hysteresis at low temperature with a coercive field of ∼0.34 T and linear dependence at high temperature corresponds to paramagnetic region. Based on the magnetic field dependence magnetization data, the maximum entropy change and relative cooling power (RCP) were estimated and the values were 1.002 J kg-1 K-1 and 90 J kg-1 for a field change of 5 T respectively. Temperature dependent resistivity ρ(T) data exhibited semiconducting-like behavior at high temperature and the electrical transport was well explained by Mott's variable-range hopping (VRH) conduction mechanism in the temperature range of 250 K-300 K. Using the VRH fit, the calculated hoping distance (Rh) at 300 K was 54.4 Å and density of states N(EF) at room temperature was 7.04 × 1018 eV-1 cm-3. These values were comparable to other semiconducting oxides.

  16. Temperature effects on the Davydov soliton

    DEFF Research Database (Denmark)

    Cruzeiro, L.; Halding, J.; Christiansen, Peter Leth

    1988-01-01

    As a possible mechanism for energy storage and transport in proteins, Davydov has proposed soliton formation and propagation. In this paper we investigate the stability of Davydov solitons at biological temperatures. From Davydov’s original theory evolution equations are derived quantum...... mechanically without approximations, and their numerical solutions at different temperatures are presented. Our conclusion is that the Davydov soliton is stable at 310 K....

  17. Finite temperature effects in primordial inflation

    Science.gov (United States)

    Gelmini, G. B.; Nanopoulos, D. V.; Olive, K. A.

    1983-11-01

    We present a detailed study of a recently proposed model for primordial inflation based on an N=1 locally supersymmetric potential. For a large class of parameters with which all cosmological constraints are satisfied, the temperature corrections can be neglected during the inflation period. At higher temperatures, the minimum is not at the origin, but very close to it. Address after July 1, 1983: Theory Group, Fermilab, PO Box 500, Batavia, IL 60510, USA.

  18. A Model-Based Temperature-Prediction Method by Temperature-Induced Spectral Variation and Correction of the Temperature Effect.

    Science.gov (United States)

    Yang, Qhi-xiao; Peng, Si-long; Shan, Peng; Bi, Yi-ming; Tang, Liang; Xie, Qiong

    2015-05-01

    In the present paper, a new model-based method was proposed for temperature prediction and correction. First, a temperature prediction model was obtained from training samples; then, the temperature of test samples were predicted; and finally, the correction model was used to reduce the nonlinear effects of spectra from temperature variations. Two experiments were used to verify the proposed method, including a water-ethanol mixture experiment and a ternary mixture experiment. The results show that, compared with classic method such as continuous piecewise direct standardization (CPDS), our method is efficient for temperature correction. Furthermore, the temperatures of test samples are not necessary in the proposed method, making it easier to use in real applications.

  19. Analyses of TmAl{sub 2} and ErAl{sub 2} composite for use as an active magnetic regenerator close to liquid helium temperature

    Energy Technology Data Exchange (ETDEWEB)

    Souza, M.V. de, E-mail: marcos_vinicios@hotmail.com [Núcleo de Pós-Graduação em Física, Campus prof. José Aluísio de Campos, UFS, 49100-000, São Cristóvão, SE (Brazil); Silva, J.A. da [Núcleo de Pós-Graduação em Física, Campus prof. José Aluísio de Campos, UFS, 49100-000, São Cristóvão, SE (Brazil); Silva, L.S. [Núcleo de Pós-Graduação em Física, Campus prof. José Aluísio de Campos, UFS, 49100-000, São Cristóvão, SE (Brazil); Instituto Federal de Tocantins, IFTO – Campus Colinas do Tocantins, AV. Bernardo Sayao S/N, Chácara Raio de Sol, Setor Santa Maria, CEP 77760-000, Colinas do Tocantins, TO (Brazil)

    2017-07-01

    Highlights: • Modeling of the thermodynamics quantities in RAl{sub 2} (R = Er, Tm) single crystal and polycrystal. • An optimal hybrid magnetocaloric material using TmAl{sub 2} and ErAl{sub 2} compounds. • Suppression of the ferromagnetic canted order in the compound TmAl{sub 2} in single crystal form. - Abstract: We report the thermodynamic properties of selected intermetallic RAl{sub 2} (R = Er, Tm) compounds calculated by using a model Hamiltonian, including the Zeeman-exchange interactions and the crystalline electrical field, which are responsible for the magnetic anisotropy. The relationship between the behavior of the temperature-dependent magnetization, calculated in different crystallographic directions for several magnetic fields, and the influence of spin reorientation on the magnetocaloric effect, is discussed. In order to validate the obtained theoretical results, experimental data are compared to calculated data. Also, an optimum molar fraction of the ErAl{sub 2} and TmAl{sub 2} composite was determined theoretically, showing a high potential for use in a regenerative thermal cycle, especially close to the liquid helium temperature range.

  20. Temperature extremes: Effect on plant growth and development

    Directory of Open Access Journals (Sweden)

    Jerry L. Hatfield

    2015-12-01

    Full Text Available Temperature is a primary factor affecting the rate of plant development. Warmer temperatures expected with climate change and the potential for more extreme temperature events will impact plant productivity. Pollination is one of the most sensitive phenological stages to temperature extremes across all species and during this developmental stage temperature extremes would greatly affect production. Few adaptation strategies are available to cope with temperature extremes at this developmental stage other than to select for plants which shed pollen during the cooler periods of the day or are indeterminate so flowering occurs over a longer period of the growing season. In controlled environment studies, warm temperatures increased the rate of phenological development; however, there was no effect on leaf area or vegetative biomass compared to normal temperatures. The major impact of warmer temperatures was during the reproductive stage of development and in all cases grain yield in maize was significantly reduced by as much as 80−90% from a normal temperature regime. Temperature effects are increased by water deficits and excess soil water demonstrating that understanding the interaction of temperature and water will be needed to develop more effective adaptation strategies to offset the impacts of greater temperature extreme events associated with a changing climate.

  1. Optimization of magnetocaloric properties of arc-melted and spark plasma-sintered LaFe{sub 11.6}Si{sub 1.4}

    Energy Technology Data Exchange (ETDEWEB)

    Shamba, P.; Morley, N.A.; Reaney, I.M.; Rainforth, W.M. [University of Sheffield, Department of Materials Science and Engineering, Sheffield (United Kingdom); Cespedes, O. [University of Leeds, School of Physics and Astronomy, Leeds (United Kingdom)

    2016-08-15

    LaFe{sub 11.6}Si{sub 1.4} alloy has been synthesized in polycrystalline form using both arc melting and spark plasma sintering (SPS). The phase formation, hysteresis loss and magnetocaloric properties of the LaFe{sub 11.6}Si{sub 1.4} alloys synthesized using the two different techniques are compared. The annealing time required to obtain the 1:13 phase is significantly reduced from 14 days (using the arc melting technique) to 30 min (using the SPS technique). The magnetic entropy change (ΔS{sub M}) for the arc-melted LaFe{sub 11.6}Si{sub 1.4} compound, obtained for a field change of 5 - 0T (decreasing field), was estimated to be 19.6 J kg{sup -1} K{sup -1}. The effective RCP at 5T of the arc-melted LaFe{sub 11.6}Si{sub 1.4} compound was determined to be 360 J kg{sup -1} which corresponds to about 88 % of that observed in Gd. A significant reduction in the hysteretic losses in the SPS LaFe{sub 11.6}Si{sub 1.4} compound was observed. The ΔS{sub M}, obtained for a field change of 5 - 0T (decreasing field), for the SPS LaFe{sub 11.6}Si{sub 1.4} compound decreases to 7.4 J kg{sup -1} K{sup -1}. The T{sub C} also shifts from 186 (arc-melted) to 230 K (SPS) and shifts the order of phase transition from first to second order, respectively. The MCE of the SPS LaFe{sub 11.6}Si{sub 1.4} compound spreads over a larger temperature range with the RCP value at 5T reaching 288 J kg{sup -1} corresponding to about 70 % of that observed in Gd. At low fields, the effective RCP values of the arc-melted and spark plasma-sintered LaFe{sub 11.6}Si{sub 1.4} compounds are comparable, thereby clearly demonstrating the potential of SPS LaFe{sub 11.6}Si{sub 1.4} compounds in low-field magnetic refrigeration applications. (orig.)

  2. The effects of incubation period and temperature on the Hydrogen ...

    African Journals Online (AJOL)

    EJIRO

    incubation period and temperature had significant effects (P = 0.05) on the efficiency of H2S technique. The times when H2S bottles take to turn ..... because at reduced temperature cellular metabolic activi- ties and growth decreases, therefore ..... that the rate of blackening depended on the concen- tration and temperature.

  3. Effect Of Oxidation Temperature And Oxidation Time On Thickness ...

    African Journals Online (AJOL)

    Investigation has been made concerning the effect of oxidation temperature and time on the thickness of copper (I) oxides solar cells prepared by thermal oxidation method. The samples were oxidized at different oxidation temperatures and time. The different oxidation temperatures and lengths of time ware employed in ...

  4. Effect of air drying temperature on rehydration ability, colour ...

    African Journals Online (AJOL)

    Effect of air drying temperature on rehydration ability, colour development and ascorbic acid content of red pepper. ... The vitamin C content of red peppers decreased linearly from 133.1 to 48.79 mg/100 g as the air-drying temperature increased from 30oC (ambient temperature) to 70o C, with a maximum loss of 63.34 ...

  5. Effects of Elevated Temperature on Compressive Strength Of Concrete

    African Journals Online (AJOL)

    This study presents the results of investigation of the effects of elevated temperatures on the compressive strength of Grade 40 concrete. A total of thirty cube specimens were cast, cured in water at ambient temperature in the laboratory and subjected to various temperature regimes before testing. A concrete mix of 1:1:3 ...

  6. EFFECT OF PREPARATION TEMPERATURE AND IONS DOPING ...

    African Journals Online (AJOL)

    B. S. Chandravanshi

    The catalytic activity of the synthesized catalysts is investigated for the reduction reaction of 4-nitrophenol ... Nanoparticles have potential applications in chemistry, physics, electronics, biology, and medicine due ... temperature on size, morphology and consequently catalytic activity of Co-B amorphous nano catalysts were ...

  7. Enhanced battery model including temperature effects

    NARCIS (Netherlands)

    Rosca, B.; Wilkins, S.

    2013-01-01

    Within electric and hybrid vehicles, batteries are used to provide/buffer the energy required for driving. However, battery performance varies throughout the temperature range specific to automotive applications, and as such, models that describe this behaviour are required. This paper presents a

  8. Le Chatelier's Principle, Temperature Effects, and Entropy.

    Science.gov (United States)

    Campbell, J. Arthur

    1985-01-01

    One of the most useful methods of understanding chemical equilibria is provided by Le Chatelier's principle. The relationships between this principle, temperature, and entropy are discussed. Tables with thermodynamic data for some net reactions commonly used to illustrate the principle and for reactions involving gases are included. (JN)

  9. Distance and temperature effects on pika forage

    Science.gov (United States)

    Jim F. Fowler; Barbara Smith; Steve Overby

    2014-01-01

    The American pika, Ochotona princeps, has been referred to as a 'canary in the coal mine' when it comes to climate change. This small rabbit relative inhabits cool alpine and subalpine mountain areas and has been shown to be sensitive to higher temperatures from both physiological experiments (Smith 1974) and from past climate transitions in the late...

  10. effects of temperature on the physicochemical properties

    African Journals Online (AJOL)

    dell

    traditionally processed vegetable oils deteriorate significantly at elevated temperatures (p < 0.05). However, the blends showed relatively better quality and stability than the unblended ones whereby the formulations of palm oil (PO) and sesame oil (SSO) appeared to be more stable than those of PO and sunflower oil (SO).

  11. Effect of Temperature and Relative Humidity on the Growth of ...

    African Journals Online (AJOL)

    The effects of temperature and relative humidity on the growth of Helminthosporium fulvum were investigated. Various temperature regimes of 10oC, 15oC, 20oC, 25oC, 30oC, 35oC and 40¢ªC were used to determine the temperature effect on the growth of H. fulvum. Maximum growth of H. fulvum was obtained at 25¢ªC ...

  12. Effect of Temperature and Relative Humidity on the Growth of ...

    African Journals Online (AJOL)

    ABSTRACT: The effects of temperature and relative humidity on the growth of Helminthosporium fulvum were investigated. Various temperature regimes of 10oC, 15oC, 20oC, 25oC, 30oC, 35oC and 40˚C were used to determine the temperature effect on the growth of H. fulvum. Maximum growth of H. fulvum was obtained ...

  13. The effects of temperature on the radiation chemistry of polymers

    International Nuclear Information System (INIS)

    Hill, D.J.T.

    1995-01-01

    The effects of high energy radiation on polymers is dependent on a number of factors. One of the most important factors is the radiolysis temperature. This paper discusses the effects of the α-transition and the other secondary transitions, as well as the ceiling and melting temperatures, on the nature of the radiolysis reactions which occur for a number of polymers. Some implications of changes in the radiation chemistry of polymers with a change in the temperature are also considered. (author)

  14. The Effect of Temperature on Moisture Transport in Concrete.

    Science.gov (United States)

    Wang, Yao; Xi, Yunping

    2017-08-09

    Most concrete structures and buildings are under temperature and moisture variations simultaneously. Thus, the moisture transport in concrete is driven by the moisture gradient as well as the temperature gradient. This paper presents an experimental approach for determining the effect of different temperature gradients on moisture distribution profiles in concrete. The effect of elevated temperatures under isothermal conditions on the moisture transport was also evaluated, and found not to be significant. The non-isothermal tests show that the temperature gradient accelerates the moisture transport in concrete. The part of increased moisture transfer due to the temperature gradient can be quantified by a coupling parameter D HT , which can be determined by the present test data. The test results indicated that D HT is not a constant but increases linearly with the temperature variation. A material model was developed for D HT based on the experimental results obtained in this study.

  15. Effect of Temperature and Hose Genotype on Components of ...

    African Journals Online (AJOL)

    Effect of Temperature and Hose Genotype on Components of Resistance to Groundnut Rust. ... African Crop Science Journal ... The effects of temperature on incubation period, infection frequency, lesion diameter, leaf area damage, pustule rupture, and sporulation were quantified for six groundnut genotypes, representing ...

  16. Theoretical analysis of effect of temperature on threshold ...

    Indian Academy of Sciences (India)

    TECS

    laser diodes, we investigated the effect of temperature on optical confinement by analysing the near field intensity. The physical parameters such as band gap energy, thresh- old current, mirror loss and others show great dependence on temperature (Patil and Gautam 2004). Hence, we took great care to explore the effect ...

  17. The effects of storage temperature and position on embryonic ...

    African Journals Online (AJOL)

    The present study was carried out with the aim of determining the effects of storage temperature and storage position on embryonic mortalities in ostrich eggs. A total of 229 ostrich eggs was collected from two commercial ostrich farms. The effects of storage temperature on embryonic mortality differed. Embryonic deaths ...

  18. Effects of temperature, light, desiccation and cold storage on ...

    African Journals Online (AJOL)

    oyaide

    2015-03-25

    Mar 25, 2015 ... Effects of light and temperature on seed germination. Light had no significant effect on seed germination at several constant temperatures (P > 0.05, Figure 1). In terms of final mean germination percentage, there was no significant difference between 15, 20, 25 and 30°C (P. > 0.05), being significant higher ...

  19. Temperature hysteretic effect and its influence on colossal ...

    Indian Academy of Sciences (India)

    has been made to study the effects of higher magnetic fields on the CMR and temperature hysteretic effects in bulk LNCMO. The motivation for this investigation is to study the effect of higher magnetic fields up to 40 kOe on bulk La0.33Nd0.33Ca0.33MnO3 sample in enhancing CMR effect up to 99% in the wide temperature ...

  20. 'Vanishing' structural effects of temperature in polymer glasses close to the glass-transition temperature

    International Nuclear Information System (INIS)

    Shantarovich, V.P.; Suzuki, T.; Ito, Y.; Yu, R.S.; Kondo, K.; Yampolskii, Yu. P.; Alentiev, A.Yu.

    2007-01-01

    Positron annihilation lifetime (PAL) measurements were used for observation of structural effects of temperature in polystyrene (PS), super-cross-linked polystyrene networks (CPS), and in polyimides (PI) below and in the vicinity of glass-transition temperature T g . 'Vanishing' of these structural effects in the repeating cycles of the temperature controlled PAL experiments due to the slow relaxation processes in different conditions and details of chemical structure is demonstrated. Obtained results illustrate complex, dependent on thermal history, inhomogeneous character of the glass structure. In fact, structure of some polymer glasses is changing continuously. Calculations of the number density of free volume holes in these conditions are discussed

  1. Effects of temperature during the irradiation of calcium carbonate

    International Nuclear Information System (INIS)

    Negron M, A.; Camargo R, C.; Ramos B, S.; Gomez V, V.; Uribe, R. M.

    2015-10-01

    The gamma irradiation of calcium carbonate at different doses (0 to 309 kGy) and temperature regimes (77 K to 298 K) was carried out to study the effects of irradiation temperature. The changes were followed by EPR spectroscopy. We observed the formation of a composite EPR spectrum even at low radiation doses and temperature. There is a strong effect on the evaluation of the radicals formed as a function of irradiation temperature, probably due to the diffusion in the frozen powder. Response curves show that this system tends to saturate at 10 MGy at 298 K. (Author)

  2. Effect of Temperature on the Aging rate of Li Ion Battery Operating above Room Temperature.

    Science.gov (United States)

    Leng, Feng; Tan, Cher Ming; Pecht, Michael

    2015-08-06

    Temperature is known to have a significant impact on the performance, safety, and cycle lifetime of lithium-ion batteries (LiB). However, the comprehensive effects of temperature on the cyclic aging rate of LiB have yet to be found. We use an electrochemistry-based model (ECBE) here to measure the effects on the aging behavior of cycled LiB operating within the temperature range of 25 °C to 55 °C. The increasing degradation rate of the maximum charge storage of LiB during cycling at elevated temperature is found to relate mainly to the degradations at the electrodes, and that the degradation of LCO cathode is larger than graphite anode at elevated temperature. In particular, the formation and modification of the surface films on the electrodes as well as structural/phase changes of the LCO electrode, as reported in the literatures, are found to be the main contributors to the increasing degradation rate of the maximum charge storage of LiB with temperature for the specific operating temperature range. Larger increases in the Warburg elements and cell impedance are also found with cycling at higher temperature, but they do not seriously affect the state of health (SoH) of LiB as shown in this work.

  3. Temperature corrections, supersymmetric effective potentials and inflation

    International Nuclear Information System (INIS)

    Binetruy, P.; Gaillard, M.K.; California Univ., Berkeley

    1985-01-01

    We calculate the one-loop temperature corrections to general potentials in N=1 supergravity, and study the conditions under which a new inflationary scenario is possible. The results are sensitive to the total number N of chiral superfields. For large N, we find that in 'hidden sector' models supersymmetry must be broken at a scale governed by the energy density of the false vacuum: msub(3/2) > or approx. 2√8π μ 2 /Msub(p), where μ approx.= (10 -3 -10 -4 )Msub(p) in typical inflationary scenarios. We also discuss an alternative picture where inflation occurs at the preonic level, before the preon-confining phase transition. (orig.)

  4. Effects of mine strata thermal behavior and mine initial temperatures on mobile refuge alternative temperature.

    Science.gov (United States)

    Yantek, D S; Yan, L; Bissert, P T; Klein, M D

    2017-04-01

    Federal regulations require the installation of refuge alternatives (RAs) in underground coal mines. Mobile RAs have a limited ability to dissipate heat, and heat buildup can lead to a life-threatening condition as the RA internal air temperature and relative humidity increase. The U.S. National Institute for Occupational Safety and Health (NIOSH) performed heat testing on a 10-person tent-type training RA and contracted ThermoAnalytics Inc. to develop a validated thermal simulation model of the tested RA. The model was used to examine the effects of the constant mine strata temperature assumption, initial mine air temperature, initial mine strata surface temperature (MSST), initial mine strata temperature at depth (MSTD) and mine strata thermal behavior on RA internal air temperature using 117 W (400 Btu/h) of sensible heat input per simulated miner. For the studied RA, when the mine strata temperature was treated as a constant, the final predicted RA internal air temperature was 7.1°C (12.8°F) lower than it was when the mine strata thermal behavior was included in the model. A 5.6°C (10.0°F) increase in the initial MSST resulted in a 3.9°C (7.1°F) increase in the final RA internal air temperature, whereas a 5.6°C (10°F) increase in the initial MSTD yielded a 1.4°C (2.5°F) increase in the final RA internal air temperature. The results indicate that mine strata temperature increases and mine strata initial temperatures must be accounted for in the physical testing or thermal simulations of RAs.

  5. Temperature, humidity and time. Combined effects on radiochromic film dosimeters

    DEFF Research Database (Denmark)

    Abdel-Fattah, A.A.; Miller, A.

    1996-01-01

    The effects of both relative humidity and temperature during irradiation on the dose response of FWT-60-00 and Riso B3 radiochromic film dosimeters have been investigated in the relative humidity (RH) range 11-94% and temperature range 20-60 degrees C for irradiation by Co-60 photons and 10-Me......V electrons. The results show that humidity and temperature cannot be treated as independent variables, rather there appears to be interdependence between absorbed dose, temperature, and humidity. Dose rate does not seem to play a significant role. The dependence of temperature during irradiation is +0.......25 +/- 0.1% per degrees C for the FWT-60-00 dosimeters and +0.5 +/- 0.1% per degrees C For Riso B3 dosimeters at temperatures between 20 and 50 degrees C and at relative humidities between 20 and 53%. At extreme conditions both with respect to temperature and to humidity, the dosimeters show much stronger...

  6. Effect of Cr substitution on magnetic and magnetic entropy change of La{sub 0.65}Eu{sub 0.05}Sr{sub 0.3}Mn{sub 1−x}Cr{sub x}O{sub 3} (0.05≤x≤0.15) rhombohedral nanocrystalline near room temperature

    Energy Technology Data Exchange (ETDEWEB)

    Bellouz, R., E-mail: bellouzridha@yahoo.fr [Laboratoire de Physico-chimie des Matériaux, Département de Physique, Faculté des Sciences de Monastir,Université de Monastir, 5019 (Tunisia); Oumezzine, M. [Laboratoire de Physico-chimie des Matériaux, Département de Physique, Faculté des Sciences de Monastir,Université de Monastir, 5019 (Tunisia); Hlil, E.K. [Institut Néel, National Centre for Scientific Research, Université Joseph Fourier, B.P. 166, 38042 Grenoble (France); Dhahri, E. [Laboratoire de Physique appliqué, Département de physique, Faculté des Sciences de Sfax, 3018 (Tunisia)

    2015-02-01

    We have studied the effect of Cr substitution on magnetic and magnetocaloric properties in nanocrystalline La{sub 0.65}Eu{sub 0.05}Sr{sub 0.3}Mn{sub 1−x}Cr{sub x}O{sub 3} (x=0.05, 0.1 and 0.15). The materials were prepared using the Pechini sol–gel method. All the studied samples were crystallized into a single phase rhombohedral structure with R−3C space group. Magnetic measurements indicate that the ferromagnetic double exchange interaction is weakened with increasing Cr concentration, resulting in a shift in T{sub C} from 338 K to 278 K as x varied between 0.05 and 0.15. Detailed analyzes in the vicinity of the ferromagnetic (FM)–paramagnetic (PM) phase-transition temperature prove the samples undergoing a second-order phase transition. The magnetocaloric effect is calculated from the measurement of initial isothermal magnetization versus magnetic field at various temperatures. The maximum magnetic entropy change |ΔS{sub M}{sup max}| is found to decrease with increasing of Cr content from 4.04 J/Kg K for x=0.05–0.78 J/KgK for x=0.15 upon 5 T applied field change. The relative cooling power (RCP) of La{sub 0.65}Eu{sub 0.05}Sr{sub 0.3}Mn{sub 1−x}Cr{sub x}O{sub 3} series is nearly 54% of pure Gd, which will be an interesting system for application in room temperature refrigeration. - Highlights: • Nanocrystalline materials La{sub 0.65}Eu{sub 0.05}Sr{sub 0.3}Mn{sub 1−x}Cr{sub x}O{sub 3} were obtained. • The Cr substitution decreases the T{sub C} from 338 K for x=0.05–278 K for x=0.15. • The relative cooling power of La{sub 0.65}Eu{sub 0.05}Sr{sub 0.3}Mn{sub 1−x}Cr{sub x}O{sub 3} is nearly 54% of pure Gd. • Arrott plot analyses was applied to study the order of the magnetic transition. • La{sub 0.65}Eu{sub 0.05}Sr{sub 0.3}Mn{sub 1−x}Cr{sub x}O{sub 3} samples show second order PM–FM transition at T=T{sub C}.

  7. Effect of monovalent doping on the physical properties of La0.7Sr0.3MnO3 compound synthesized using sol-gel technique

    Science.gov (United States)

    Ayadi, F.; Saadaoui, F.; Cheikhrouhou-Koubaa, W.; Koubaa, M.; Cheikhrouhou, A.; Sicard, L.; Ammar, S.

    2012-02-01

    In this work, we have studied the effect of monovalent substitution on the structural, magnetic and magnetocaloric properties of the P-doped La0.7Sr0.2M0.1MnO3 (M = Na, K) manganites synthesized by sol-gel technique. Structural investigations using X-ray diffraction show that all the elaborated compounds crystallize in the rhomboedral structure with R-3c space group. The increase in the ionic radius induces a rotation of MnO6 octahedra leading to a change in the Mn-O-Mn angles and the Mn-O distances. Magnetizations measurements were carried out using vibrating sample magnetometer operating above room temperature with magnetic applied field up to 5 tesla. All our samples exhibit paramagnetic to ferromagnetic transition with a Curie temperature above room temperature. From magnetic measurements versus magnetic applied field at several temperatures, we have determined the magnetocaloric effect using the classical thermodynamics based on Maxwell relations.

  8. Magnetocaloric properties of Ag-substituted perovskite-type manganites

    International Nuclear Information System (INIS)

    Tang, T.; Gu, K.M.; Cao, Q.Q.; Wang, D.H.; Zhang, S.Y.; Du, Y.W.

    2000-01-01

    Magnetic entropy change larger than that of gadolinium has been observed near room temperature in polycrystalline of La 0.8 Ag 0.2 MnO 3 perovskite-type manganite. The large magnetic entropy change produced by the abrupt reduction of magnetization is associated with a first-order phase transition of the sample near the Curie temperature. This phenomenon indicates that perovskite manganites have some potential applications for magnetic refrigerants in an extended high-temperature range

  9. Microstructural Evolution and Mechanical Behavior of High Temperature Solders: Effects of High Temperature Aging

    Science.gov (United States)

    Hasnine, M.; Tolla, B.; Vahora, N.

    2018-04-01

    This paper explores the effects of aging on the mechanical behavior, microstructure evolution and IMC formation on different surface finishes of two high temperature solders, Sn-5 wt.% Ag and Sn-5 wt.% Sb. High temperature aging showed significant degradation of Sn-5 wt.% Ag solder hardness (34%) while aging has little effect on Sn-5 wt.% Sb solder. Sn-5 wt.% Ag experienced rapid grain growth as well as the coarsening of particles during aging. Sn-5 wt.% Sb showed a stable microstructure due to solid solution strengthening and the stable nature of SnSb precipitates. The increase of intermetallic compound (IMC) thickness during aging follows a parabolic relationship with time. Regression analysis (time exponent, n) indicated that IMC growth kinetics is controlled by a diffusion mechanism. The results have important implications in the selection of high temperature solders used in high temperature applications.

  10. Hydrostatic pressure effect on the spin reorientation transition of ferromagnetic Sm0.7-xLaxSr0.3MnO3 (x = 0, 0.1) polycrystals

    Science.gov (United States)

    Thiyagarajan, R.; Arumugam, S.; Sivaprakash, P.; Kannan, M.; Saravanan, C.; Yang, Wenge

    2017-06-01

    The hydrostatic pressure effect on the resistivity and magnetization of the narrow band gap manganite Sm0.7-xLaxSr0.3MnO3 (x = 0, 0.1) systems has been investigated. At ambient pressure measurements, the parent compound Sm0.7Sr0.3MnO3 showed a ferromagnetic-insulating nature, whereas the 10% La-doped compound Sm0.6La0.1Sr0.3MnO3 showed a ferromagnetic-metallic nature. Furthermore, both samples showed a spin-reorientation transition (TSR) below Curie temperature, which originated from the Mn sublattice and was supported by an antiferromagnetic Sm(4f)-Mn(3d) interaction. Both samples exhibited a normal and inverse magnetocaloric effect as a result of these two different magnetic transitions. Magnetization measurements on Sm0.7Sr0.3MnO3 under pressure did not show an appreciable change in the Curie temperature, but enhanced TSR, whereas an insulator-metallic transition was observed during resistivity measurements under pressure. On the other hand, for Sm0.6La0.1Sr0.3MnO3, TC increased and TSR reduced upon the application of pressure. The metallic nature which is observed at ambient pressure resistivity measurement was further enhanced with 97% of piezoresistance. The pressure did not change the normal magnetocaloric effect of Sm0.7Sr0.3MnO3, but increased it in Sm0.6La0.1Sr0.3MnO3. However, there was not much change in the inverse magnetocaloric effect of both compounds. These studies were analyzed based on the pressure effect on the activation energy and scattering interaction factors.

  11. Effect of temperature on seed production in the invasive grass ...

    African Journals Online (AJOL)

    Temperature is one of the main factors that determine sexual reproduction in terrestrial and emergent aquatic plant species. The effect of temperature on sexual reproduction and seed production of Glyceria maxima (Hartm.) Holmb. in the southern hemisphere is unknown. Glyceria maxima collections in February 2010 at ...

  12. Effect of temperature on structure and corrosion resistance for ...

    Indian Academy of Sciences (India)

    Abstract. The effect of plating temperatures between 60 and 90◦C on structure and corrosion resistance for elec- troless NiWP coatings on AZ91D magnesium alloy substrate was investigated. Results show that temperature has a significant influence on the surface morphology and corrosion resistance of the NiWP alloy ...

  13. Effect of isotopy and temperature on hydration of alkanols

    Energy Technology Data Exchange (ETDEWEB)

    Korolev, V.P.; Batov, D.V.; Krestov, G.A.

    1987-07-10

    The authors determine isotope and temperature effects on the hydration of alkanols at a temperature of 278.15 K in solutions of water and heavy water. Aspects of isotopic exchange between hydrogen and deuterium are given as are enthalpies of hydration, evaporation, and dissolution for the alkanols. The possibility of weak hydrogen bond formation was examined.

  14. Effect of temperature on the AC impedance of protein and ...

    Indian Academy of Sciences (India)

    increased with temperature for all the biopolymers which corresponds to high polarization effect in these biopoly- mers. The AC impedance parameters for papain, gum aca- cia, gum tragacanth and gum guar are given for four different temperatures in table 1 for comparison. The conductivity of papain increases from 1·65× ...

  15. Effect of oxidation and annealing temperature on optical and ...

    Indian Academy of Sciences (India)

    Administrator

    Abstract. Tin oxide thin films were deposited on glass substrate with 100 nm thickness of Sn, which was coated by magnetron sputtering followed by thermal oxidation at different temperatures. The effect of oxidation temperature on the optical and structural properties of SnO2 films were investigated. Higher transmittance ...

  16. Effect of temperature on structure and corrosion resistance for ...

    Indian Academy of Sciences (India)

    The effect of plating temperatures between 60 and 90 ∘ C on structure and corrosion resistance for electroless NiWP coatings on AZ91D magnesium alloy substrate was investigated. Results show that temperature has a significant influence on the surface morphology and corrosion resistance of the NiWP alloy coating.

  17. Effect of temperature shocks on membrane fouling in membrane bioreactors

    NARCIS (Netherlands)

    Brink, van den P.; Satpradit, O.A.; Bentem, van A.; Zwijnenburg, A.; Temmink, B.G.; Loosdrecht, M.C.M.

    2011-01-01

    Temperature is known to influence the biological performance of conventional activated sludge systems. In membrane bioreactors (MBRs), temperature not only affects the bioconversion process but is also shown to have an effect on the membrane performance. Four phenomena are generally reported to

  18. Temperature effects on quantum interference in molecular junctions

    DEFF Research Database (Denmark)

    Markussen, Troels; Thygesen, Kristian Sommer

    2014-01-01

    A number of experiments have demonstrated that destructive quantum interference (QI) effects in molecular junctions lead to very low conductances even at room temperature. On the other hand, another recent experiment showed increasing conductance with temperature which was attributed to decoherence...

  19. Effects of Decortication Temperature on the Functional Properties of ...

    African Journals Online (AJOL)

    The effects of decortication temperature on the functional and sensory properties of the cowpea flour (Vigna unguiculata) and steam flour paste were studied. Cowpea seeds were soaked at different temperatures (20oC, 40oC, 60oC, 80oC and 100oC) prior to decortication. The functional properties of the cowpea flour, ...

  20. Effect of Calcination and Reduction Temperatures on the Reduction ...

    African Journals Online (AJOL)

    The effect of calcination and reduction temperatures on the reducibility, dispersion and Fischer-Tropsch activity of 10 wt% cobalt supported on titania catalyst modified by 0.1 wt% boron has been studied. The percentage reduction and percentage dispersion were found to decrease with increasing calcination temperature.

  1. On the effect of temperature dependent thermal conductivity on ...

    African Journals Online (AJOL)

    We consider the effect of temperature dependent thermal conductivity on temperature rise in biologic tissues during microwave heating. The method of asymptotic expansion is used for finding solution. An appropriate matching procedure was used in our method. Our result reveals the possibility of multiple solutions and it ...

  2. Possible effects of regulating hydroponic water temperature on plant ...

    African Journals Online (AJOL)

    Yomi

    2010-12-29

    Dec 29, 2010 ... on the production of chlorophyll pigments in plants grown during the winter period. POSSIBLE EFFECTS OF REGULATING HYDROPONIC. WATER TEMPERATURE REGIMES ON THE. PHOTOSYNTHESIS RATE. Temperature is an important environmental factor to plants, which directly influences their ...

  3. Effects of preparation temperature on the conductivity of polypyrrole ...

    Indian Academy of Sciences (India)

    An attempt has been made to investigate the effect of temperature on the conductivity of polypyrrole conducting polymer films prepared by an electrochemical method in an aqueous medium using camphor sulfonate as the dopant. The polymer was grown from aqueous solutions employing a range of temperatures (1-60°C).

  4. Effect of Temperature on the Oviposition Capacity of Engorged Adult ...

    African Journals Online (AJOL)

    Effects of temperature on the oviposition capacity of engorged adult females of Rhipicephalus sanguineus and Haemaphysalis leachi leachi and on the hatching pattern of their eggs were investigated under laboratory conditions. The temperatures of maintenance were 150C, 200C, 250C, 300C and 370C at 85% relative ...

  5. Effects of temperature and growing seasons on crop water ...

    African Journals Online (AJOL)

    Through shifting growing seasons and minimizing the effects of temperature for the major crops, significant amount of groundwater may be saved, which can reduce the production of costly desalinated water. Keywords: Water resources; conservation; crop water requirement; temperature; growing seasons; policy ...

  6. Effect of temperature on shelf life, chemical and microbial properties ...

    African Journals Online (AJOL)

    Cream cheese samples were analyzed to find out the effect of recommended storage temperature (4±1°C) and ambient room temperature (21±1°C) on pH, titratable acidity (% lactic acid), moisture content and microbial growth. Percent reduction in moisture content and increase in titratable acidity of cheeses were found to ...

  7. Effect of temperature on moromi fermentation of soy sauce with ...

    African Journals Online (AJOL)

    It was learned that as the aging of moromi took place, the pH level was decreased from pH 7 to 4.88. Also, the soy sauce had lower concentration of ethanol when higher temperature was used in moromi fermentation but the difference of temperature did not show significantly effect on total nitrogen content in soy sauce.

  8. Effects of exhaust temperature on helicopter infrared signature

    International Nuclear Information System (INIS)

    Cheng-xiong, Pan; Jing-zhou, Zhang; Yong, Shan

    2013-01-01

    The effects of exhaust temperature on infrared signature (in 3–5 μm band) for a helicopter equipped with integrative infrared suppressor were numerically investigated. The internal flow of exhaust gas and the external downwash flow, as well as the mixing between exhaust gas and downwash were simulated by CFD software to determine the temperature distributions on the helicopter skin and in the exhaust plume. Based on the skin and plume temperature distributions, a forward–backward ray-tracing method was used to calculate the infrared radiation intensity from the helicopter with a narrow-band model. The results show that for a helicopter with its integrative infrared suppressor embedded inside its rear airframe, the exhaust temperature has significant influence on the plume radiation characteristics, while the helicopter skin radiation intensity has little impact. When the exhaust temperature is raised from 900 K to 1200 K, the plume radiation intensity in 3–5 μm band is increased by about 100%, while the skin radiation intensity is increased by only about 5%. In general, the effects of exhaust temperature on helicopter infrared radiation intensity are mainly concentrated on plume, especially obvious for a lower skin emissivity case. -- Highlights: ► The effect of exhaust temperature on infrared signature for a helicopter is numerically investigated. ► The impact of exhaust temperature on helicopter skin temperature is revealed. ► The impact of exhaust temperature on plume radiation characteristics is revealed. ► The impact of exhaust temperature on helicopter skin radiation is revealed. ► The impact of exhaust temperature on helicopter's total infrared radiation intensity is revealed

  9. Structural, magnetic and magnetocaloric properties of polycrystalline La{sub 0.67}Ba{sub 0.33-x}Zn{sub x}MnO{sub 3} (x = 0.15 and 0.2) manganites

    Energy Technology Data Exchange (ETDEWEB)

    Zaidi, Asma; Mohamed, Z.; Dhahri, J. [University of Monastir, Laboratory of Condensed Matter and Nanosciences, Monastir (Tunisia); Hlil, E.K. [CNRS, University of Joseph Fourier, Institut Neel, Grenoble (France); Alharbi, T.; Zaidi, M. [Majmaah University, College of Science of Zulfi, Al Majmaah (Saudi Arabia)

    2016-04-15

    We report on the structural, magnetic and magnetocaloric properties of manganite La{sub 0.67}Ba{sub 0.33-x}Zn{sub x}MnO{sub 3} (x=0.15 and 0.2). X-ray diffraction studies show that all samples crystallize with the rhombohedral symmetry within the space group R anti 3c. The magnetic and magnetocaloric properties of polycrystalline perovskite were investigated from the measured magnetization data of the samples as a function of the applied magnetic field. The associated magnetic entropy change close to their respective Curie temperature T{sub C} and the relative cooling power (RCP) have been determined. It was found that the maximum change in magnetic entropy of La{sub 0.67}Ba{sub 0.33-x}Zn{sub x}MnO{sub 3} samples reached 3.4 J/kg K at T{sub C}=260 K for a magnetic field of 5 T and RCP=223.77 J/kg. In view of these results, La{sub 0.67}Ba{sub 0.33-x}Zn{sub x}MnO{sub 3} compounds are potential candidates for magnetic refrigeration. (orig.)

  10. Temperature effects on neutron drip line

    International Nuclear Information System (INIS)

    Rajasekaran, M.; Aggarwal, Mamta

    1996-01-01

    Extremely neutron rich hot nuclei formed in high energy collisions having high thermal excitation energies are investigated in the framework of statistical theory and the effect of level density parameter a = U/T 2 , on the drip line is analysed

  11. Modeling the Temperature Effect of Orientations in Residential Buildings

    Directory of Open Access Journals (Sweden)

    Sabahat Arif

    2012-07-01

    Full Text Available Indoor thermal comfort in a building has been an important issue for the environmental sustainability. It is an accepted fact that their designs and planning consume a lot of energy in the modern architecture of 20th and 21st centuries. An appropriate orientation of a building can provide thermally comfortable indoor temperatures which otherwise can consume extra energy to condition these spaces through all the seasons. This experimental study investigates the potential effect of this solar passive design strategy on indoor temperatures and a simple model is presented for predicting indoor temperatures based upon the ambient temperatures.

  12. Temperature effects on gallium arsenide 63Ni betavoltaic cell.

    Science.gov (United States)

    Butera, S; Lioliou, G; Barnett, A M

    2017-07-01

    A GaAs 63 Ni radioisotope betavoltaic cell is reported over the temperature range 70°C to -20°C. The temperature effects on the key cell parameters were investigated. The saturation current decreased with decreased temperature; whilst the open circuit voltage, the short circuit current, the maximum power and the internal conversion efficiency values decreased with increased temperature. A maximum output power and an internal conversion efficiency of 1.8pW (corresponding to 0.3μW/Ci) and 7% were observed at -20°C, respectively. Copyright © 2017 The Authors. Published by Elsevier Ltd.. All rights reserved.

  13. Local and effective temperatures of quantum driven systems

    Science.gov (United States)

    Caso, Alvaro; Arrachea, Liliana; Lozano, Gustavo S.

    2010-01-01

    We introduce thermometers to define the local temperature of an electronic system driven out of equilibrium by local ac fields. We also define the effective temperature in terms of a local fluctuation-dissipation relation. We show that within the weak driving regime these two temperatures coincide. We also discuss the behavior of the local temperature along the sample. We show that it exhibits spatial fluctuations following an oscillatory pattern. For weak driving, regions of the sample become heated, while others become cooled as a consequence of the driving.

  14. Interactive effects of temperature and habitat complexity on freshwater communities.

    Science.gov (United States)

    Scrine, Jennifer; Jochum, Malte; Ólafsson, Jón S; O'Gorman, Eoin J

    2017-11-01

    Warming can lead to increased growth of plants or algae at the base of the food web, which may increase the overall complexity of habitat available for other organisms. Temperature and habitat complexity have both been shown to alter the structure and functioning of communities, but they may also have interactive effects, for example, if the shade provided by additional habitat negates the positive effect of temperature on understory plant or algal growth. This study explored the interactive effects of these two major environmental factors in a manipulative field experiment, by assessing changes in ecosystem functioning (primary production and decomposition) and community structure in the presence and absence of artificial plants along a natural stream temperature gradient of 5-18°C. There was no effect of temperature or habitat complexity on benthic primary production, but epiphytic production increased with temperature in the more complex habitat. Cellulose decomposition rate increased with temperature, but was unaffected by habitat complexity. Macroinvertebrate communities were less similar to each other as temperature increased, while habitat complexity only altered community composition in the coldest streams. There was also an overall increase in macroinvertebrate abundance, body mass, and biomass in the warmest streams, driven by increasing dominance of snails and blackfly larvae. Presence of habitat complexity, however, dampened the strength of this temperature effect on the abundance of macroinvertebrates in the benthos. The interactive effects that were observed suggest that habitat complexity can modify the effects of temperature on important ecosystem functions and community structure, which may alter energy flow through the food web. Given that warming is likely to increase habitat complexity, particularly at higher latitudes, more studies should investigate these two major environmental factors in combination to improve our ability to predict the

  15. Effects of temperature on fluorescence in human tissue

    Science.gov (United States)

    Masters, D. B.; Walsh, Alex; Welch, A. J.; Mahadevan-Jansen, Anita

    2010-02-01

    The fluorescence properties of human tissue are known to be temperature dependent. The most apparent effect of this dependence is the inverse relationship between fluorescence and temperature. In this study, we used fluorescence and diffuse-reflectance spectroscopy to investigate the effects of temperature on fluorescence, thermal coagulation, and tissue optical properties. Human tissue from the breast and abdomen were examined in vitro, and human skin was examined in vivo using a fluorescence and diffuse-reflectance system to observe the effects of temperature on fluorescence and optical properties. Fluorescence measurements were carried out using a pulsed nitrogen laser at 337 nm for excitation and a thermal camera for temperature measurements. Thermal variation of the specimens was provided by a phosphate buffered saline solution for the in vitro experiments and an ice pack and heat lamp for the in vivo experiments. In vitro temperatures varied from 0°C to 70°C and in vivo temperatures varied from 15°C to 40°C. Optical property measurements and Monte Carlo simulations were carried out on the in vitro samples for different levels of thermal exposure. Results of both the in vivo and in vitro experiments indicate that optical properties of human tissue change at high temperatures, primarily due to increased scattering. In addition, certain internal processes may have contributed to a decrease in fluorescence with increasing temperature. Some of these effects were found to be reversible before a certain temperature threshold, while some effects of coagulation on fluorescence and optical properties were not reversible.

  16. Peltier Effect Based Temperature Controlled System for Dielectric Spectroscopy

    Science.gov (United States)

    Mukda, T.; Jantaratana, P.

    2017-09-01

    The temperature control system was designed and built for application in dielectric spectroscopy. It is based on the dual-stage Peltier element that decreases electrical power and no cryogenic fluids are required. A proportional integral derivative controller was used to keep the temperature stability of the system. A Pt100 temperature sensor was used to measure temperature of the sample mounting stage. Effect of vacuum isolation and water-cooling on accuracy and stability of the system were also studied. With the incorporation of vacuum isolation and water-cooling at 18 °C, the temperature of the sample under test can be controlled in the range of -40 °C to 150 °C with temperature stability ± 0.025 °C.

  17. Temperature Dependence of the Resonant Magnetoelectric Effect in Layered Heterostructures

    Directory of Open Access Journals (Sweden)

    Dmitrii A. Burdin

    2017-10-01

    Full Text Available The dependence of the resonant direct magnetoelectric effect on temperature is studied experimentally in planar composite structures. Samples of rectangular shapes with dimensions of 5 mm × 20 mm employed ferromagnetic layers of either an amorphous (metallic glass alloy or nickel with a thickness of 20–200 μm and piezoelectric layers of single crystalline langatate material or lead zirconate titanate piezoelectric ceramics with a thickness of 500 μm. The temperature of the samples was varied in a range between 120 and 390 K by blowing a gaseous nitrogen stream around them. It is shown that the effective characteristics of the magnetoelectric effect—such as the mechanical resonance frequency fr, the quality factor Q and the magnitude of the magnetoelectric coefficient αE at the resonance frequency—are contingent on temperature. The interrelations between the temperature changes of the characteristics of the magnetoelectric effect and the temperature variations of the following material parameters—Young’s modulus Y, the acoustic quality factor of individual layers, the dielectric constant ε, the piezoelectric modulus d of the piezoelectric layer as well as the piezomagnetic coefficients λ(n of the ferromagnetic layer—are established. The effect of temperature on the characteristics of the nonlinear magnetoelectric effect is observed for the first time. The results can be useful for designing magnetoelectric heterostructures with specified temperature characteristics, in particular, for the development of thermally stabilized magnetoelectric devices.

  18. Theory of the superconducting proximity effect below the transition temperature

    International Nuclear Information System (INIS)

    Silvert, W.

    1975-01-01

    The form of the low-temperature theory of the superconducting proximity effect depends on whether the non-linear terms are assumed to depend only on the local value of the gap or on its average value over some finite range. The local assumption leads to smaller values of the gap and to unphysical results at low temperatures. The effect of non-locality is significant even in the Ginsburg-Landau regime. (author)

  19. The crystal and magnetic structure of the magnetocaloric compound FeMnP(0.5)Si(0.5)

    Czech Academy of Sciences Publication Activity Database

    Hoglin, V.; Hudl, M.; Sahlberg, M.; Nordblad, P.; Beran, Přemysl; Anderson, I.

    2011-01-01

    Roč. 184, č. 9 (2011), s. 2434-2438 ISSN 0022-4596 Institutional research plan: CEZ:AV0Z10480505 Keywords : Magnetocaloric * Neutron powder diffraction * X-ray diffraction (XRD) * Magnetic refrigeration * Magnetic structure Subject RIV: CA - Inorganic Chemistry Impact factor: 2.159, year: 2011

  20. Chiral symmetry and finite temperature effects in quantum theories

    International Nuclear Information System (INIS)

    Larsen, Aa.

    1987-01-01

    A computer simulation of the harmonic oscillator at finite temperature has been carried out, using the Monte Carlo Metropolis algorithm. Accurate results for the energy and fluctuations have been obtained, with special attention to the manifestation of the temperature effects. Varying the degree of symmetry breaking, the finite temperature behaviour of the asymmetric linear model in a linearized mean field approximation has been studied. In a study of the effects of chiral symmetry on baryon mass splittings, reasonable agreement with experiment has been obtained in a non-relativistic harmonic oscillator model

  1. High temperature effects on compact-like structures

    Energy Technology Data Exchange (ETDEWEB)

    Bazeia, D.; Lima, E.E.M.; Losano, L. [Universidade Federal da Paraiba, Departamento de Fisica, Joao Pessoa, PB (Brazil)

    2016-08-15

    In this work we investigate the transition from kinks to compactons at high temperatures. We deal with a family of models, described by a real scalar field with standard kinematics, controlled by a single parameter, real and positive. The family of models supports kink-like solutions, and the solutions tend to become compact when the parameter increases to larger and larger values. We study the one-loop corrections at finite temperature, to see how the thermal effects add to the effective potential. The results suggest that the symmetry is restored at very high temperatures. (orig.)

  2. Temperature dependence of the elastocaloric effect in natural rubber

    Energy Technology Data Exchange (ETDEWEB)

    Xie, Zhongjian, E-mail: zhongjian.xie521@gmail.com; Sebald, Gael; Guyomar, Daniel

    2017-07-12

    The temperature dependence of the elastocaloric (eC) effect in natural rubber (NR) has been studied. This material exhibits a large eC effect over a broad temperature range from 0 °C to 49 °C. The maximum adiabatic temperature change (ΔT) occurred at 10 °C and the behavior could be predicted by the temperature dependence of the strain-induced crystallization (SIC) and the temperature-induced crystallization (TIC). The eC performance of NR was then compared with that of shape memory alloys (SMAs). This study contributes to the SIC research of NR and also broadens the application of elastomers. - Highlights: • A large elastocaloric effect over a broad temperature range was found in natural rubber (NR). • The caloric performance of NR was compared with that of shape memory alloys. • The temperature dependence of the elastocaloric effect in NR can be prediced by the theory of strain-induced crystallization.

  3. Effects of temperature on consumer-resource interactions.

    Science.gov (United States)

    Amarasekare, Priyanga

    2015-05-01

    Understanding how temperature variation influences the negative (e.g. self-limitation) and positive (e.g. saturating functional responses) feedback processes that characterize consumer-resource interactions is an important research priority. Previous work on this topic has yielded conflicting outcomes with some studies predicting that warming should increase consumer-resource oscillations and others predicting that warming should decrease consumer-resource oscillations. Here, I develop a consumer-resource model that both synthesizes previous findings in a common framework and yields novel insights about temperature effects on consumer-resource dynamics. I report three key findings. First, when the resource species' birth rate exhibits a unimodal temperature response, as demonstrated by a large number of empirical studies, the temperature range over which the consumer-resource interaction can persist is determined by the lower and upper temperature limits to the resource species' reproduction. This contrasts with the predictions of previous studies, which assume that the birth rate exhibits a monotonic temperature response, that consumer extinction is determined by temperature effects on consumer species' traits, rather than the resource species' traits. Secondly, the comparative analysis I have conducted shows that whether warming leads to an increase or decrease in consumer-resource oscillations depends on the manner in which temperature affects intraspecific competition. When the strength of self-limitation increases monotonically with temperature, warming causes a decrease in consumer-resource oscillations. However, if self-limitation is strongest at temperatures physiologically optimal for reproduction, a scenario previously unanalysed by theory but amply substantiated by empirical data, warming can cause an increase in consumer-resource oscillations. Thirdly, the model yields testable comparative predictions about consumer-resource dynamics under alternative

  4. Effect of temperature on task performance in officeenvironment

    Energy Technology Data Exchange (ETDEWEB)

    Seppanen, Olli; Fisk, William J.; Lei, Q.H.

    2006-07-01

    Indoor temperature is one of the fundamental characteristics of the indoor environment. It can be controlled with a degree of accuracy dependent on the building and its HVAC system. The indoor temperature affects several human responses, including thermal comfort, perceived air quality, sick building syndrome symptoms and performance at work. In this study, we focused on the effects of temperature on performance at office work. We included those studies that had used objective indicators of performance that are likely to be relevant in office type work, such as text processing, simple calculations (addition, multiplication), length of telephone customer service time, and total handling time per customer for call-center workers. We excluded data from studies of industrial work performance. We calculated from all studies the percentage of performance change per degree increase in temperature, and statistically analyzed measured work performance with temperature. The results show that performance increases with temperature up to 21-22 C, and decreases with temperature above 23-24 C. The highest productivity is at temperature of around 22 C. For example, at the temperature of 30 C, the performance is only 91.1% of the maximum i.e. the reduction in performance is 8.9%

  5. Temperature effect compensation for fast differential pressure decay testing

    International Nuclear Information System (INIS)

    Shi, Yan; Tong, Xiaomeng; Cai, Maolin

    2014-01-01

    To avoid the long temperature recovery period with differential pressure decay for leak detection, a novel method with temperature effect compensation is proposed to improve the testing efficiency without full stabilization of temperature. The mathematical model of conventional differential pressure decay testing is established to analyze the changes of temperature and pressure during the measuring period. Then the differential pressure is divided into two parts: the exponential part caused by temperature recovery and the linear part caused by leak. With prior information obtained from samples, parameters of the exponential part can be identified precisely, and the temperature effect will be compensated before it fully recovers. To verify the effect of the temperature compensated method, chambers with different volumes are tested under various pressures and the experiments show that the improved method is faster with satisfactory precision, and an accuracy less than 0.25 cc min −1  can be achieved when the compensation time is proportional to four times the theoretical thermal-time constant. (paper)

  6. The effectiveness of dispersants under various temperature and salinity regimes

    International Nuclear Information System (INIS)

    Fingas, M.; Fieldhouse, B.; Wang, Z.; Environment Canada, Ottawa, ON

    2005-01-01

    A series of tests were conducted to determine the effectiveness of dispersants in Arctic waters where salinity and temperature interactions play a critical role. In particular, Corexit 9500 was tested on Alaska North Slope oil at different temperatures and salinity using the ASTM standard test and variations of this test. Results were compared to the only historically reported test in which both temperature and salinity were changed over a range of values. This series of tests demonstrated that there is an interaction between salinity, temperature and dispersant effectiveness. It was shown that conventional and currently available dispersants are nearly ineffective at 0 salinity. Dispersant effectiveness peaks at 20 to 40 units of salinity, depending on the type of dispersant. Corexit is less sensitive to salinity, while Corexit 9527 is more sensitive to salinity. There is a smooth gradient of effectiveness with salinity both as the salinity rises to a peak point of effectiveness and as it exceeds this value. Results from the 2 field trials in fresh water suggest that laboratory tests correctly conclude that the effectiveness of dispersants is very low in freshwater. The study also examined several analytical factors such as the total petroleum hydrocarbon (TPH) versus relative petroleum hydrocarbon (RPH) methods, specific versus general calibration curves, and automatic versus manual baseline placement. The analytical variations of effectiveness by RPH or TPH methods do not affect the fundamental relationship between salinity and temperature. 6 refs., 6 tabs., 8 figs

  7. Analysis of Low Temperature Preheating Effect Based on Battery Temperature-Rise Model

    Directory of Open Access Journals (Sweden)

    Xiaogang Wu

    2017-08-01

    Full Text Available It is difficult to predict the heating time and power consumption associated with the self-heating process of lithium-ion batteries at low temperatures. A temperature-rise model considering the dynamic changes in battery temperature and state of charge is thus proposed. When this model is combined with the ampere-hour integral method, the quantitative relationship among the discharge rate, heating time, and power consumption, during the constant-current discharge process in an internally self-heating battery, is realized. Results show that the temperature-rise model can accurately reflect actual changes in battery temperature. The results indicate that the discharge rate and the heating time present an exponential decreasing trend that is similar to the discharge rate and the power consumption. When a 2 C discharge rate is selected, the battery temperature can rise from −10 °C to 5 °C in 280 s. In this scenario, power consumption of the heating process does not exceed 15% of the rated capacity. As the discharge rate gradually reduced, the heating time and power consumption of the heating process increase slowly. When the discharge rate is 1 C, the heating time is more than 1080 s and the power consumption approaches 30% of the rated capacity. The effect of discharge rate on the heating time and power consumption during the heating process is significantly enhanced when it is less than 1 C.

  8. Temperature effects on radiation damage in plastic detectors

    International Nuclear Information System (INIS)

    Mendoza A, D.

    1996-01-01

    The objective of present work was to study the temperature effect on radiation damage registration in the structure of a Solid State Nuclear Track Detector of the type CR-39. In order to study the radiation damage as a function of irradiation temperature, sheets of CR-39 detectors were irradiated with electron beams, simulating the interaction of positive ions. CR-39 detectors were maintained at a constant temperature from room temperature up to 373 K during irradiation. Two techniques were used from analyzing changes in the detector structure: Electronic Paramagnetic Resonance (EPR) and Infrared Spectroscopy (IR). It was found by EPR analysis that the amount of free radicals decrease as irradiation temperature increases. The IR spectrums show yield of new functional group identified as an hydroxyl group (OH). A proposed model of interaction of radiation with CR-39 detectors is discussed. (Author)

  9. Effective closure temperature in leaky and/or saturating thermochronometers

    DEFF Research Database (Denmark)

    Guralnik, Benny; Jain, Mayank; Herman, Frédéric

    2013-01-01

    (present-day) temperature TP. A subsequent extension (Ganguly and Tirone, 1999) provided a simple correction for systems cooling from an arbitrary T0, at which presence of an initial concentration profile may affect final concentrations. Here, we use a combination of analytical and numerical solutions......The classical equation of closure temperature (TC) in thermochronometry (Dodson, 1973), assumed (i) no storage limitation for the accumulating radiogenic product, (ii) a negligible product concentration at the initial temperature of cooling T0, and (iii) a negligible product loss at the final...... to derive a general expression for the effective closure temperature in (i) systems which cool between arbitrary initial and final temperatures, potentially still suffering from thermal product loss at TP (termed ‘leaky’), and (ii) systems which may contain a physical limit on the maximum amount of product...

  10. Preparation of nanostructured La{sub 0.7}Ca{sub 0.3−x}Ba{sub x}MnO{sub 3} ceramics by a combined sol–gel and spark plasma sintering route and resulting magnetocaloric properties

    Energy Technology Data Exchange (ETDEWEB)

    Ayadi, F.; Regaieg, Y. [Université Paris Diderot, Sorbonne Paris Cité, ITODYS, UMR 7086 CNRS, 15 rue J.-A. de Baïf, 75205 Paris Cedex 13 (France); Faculté des Sciences de Sfax, Université de Sfax, LPM, B.P 1171, 3000 Sfax (Tunisia); Cheikhrouhou-Koubaa, W.; Koubaa, M.; Cheikhrouhou, A. [Faculté des Sciences de Sfax, Université de Sfax, LPM, B.P 1171, 3000 Sfax (Tunisia); Lecoq, H.; Nowak, S.; Ammar, S. [Université Paris Diderot, Sorbonne Paris Cité, ITODYS, UMR 7086 CNRS, 15 rue J.-A. de Baïf, 75205 Paris Cedex 13 (France); Sicard, L., E-mail: lorette.sicard@univ-paris-diderot.fr [Université Paris Diderot, Sorbonne Paris Cité, ITODYS, UMR 7086 CNRS, 15 rue J.-A. de Baïf, 75205 Paris Cedex 13 (France)

    2015-05-01

    This work proposes an original, easy to achieve and inexpensive route to synthesize manganite ceramics for magnetic refrigeration, combining sol–gel chemistry to Spark Plasma Sintering (SPS). The target La{sub 0.7}Ca{sub 0.3−x}Ba{sub x}MnO{sub 3} (x=0, 0.1, 0.2) compounds are obtained as single phases which crystallize in the orthorhombic structure (Pnma space group). SPS allows a quick sintering at a relatively low temperature (700 °C in this work) compared to the conventional solid state method (≥1100 °C), leading to densified ultrafine grained pellets (85% of compactness). Magnetic studies show that Ba substitution does not affect significantly the relative cooling power (RCP) of these manganites, while it increases their Curie temperature (T{sub C}) by several tens of degrees. Typically, RCP values ranging between 267 and 270 J/kg (for a magnetic field change of 5 T) and T{sub C} between 205 and 245 K were measured when x was increased from 0 to 0.2, respectively. These results combined to the fact that the synthesis route is economically advantageous makes the obtained ceramics interesting as active refrigerants for magnetic refrigeration technology below room temperature. - Highlights: • Nanostructured La{sub 0.7}Ca{sub 0.3−x}Ba{sub x}MnO{sub 3} ceramics were obtained as single phase. • An original and low cost method was developed combining sol–gel chemistry and SPS. • The method can be extended to prepare most dense nanostructured oxides. • Our ceramics have higher RCP than those obtained by the solid state method. • The optimum temperature of the magnetocaloric effect is tunable with Ba content.

  11. Effect of co-site dilution on the magnetism of RCo5 (R = Gd, Y) compounds

    Science.gov (United States)

    Nikitin, S. A.; Bogdanov, A. E.; Morozkin, A. V.; Knotko, A. V.; Yapaskurt, V. O.; Ovchenkova, I. A.; Smirnov, A. V.; Nirmala, R.; Quezado, S.; Malik, S. K.

    2018-03-01

    The magnetic and magnetocaloric properties of the RCo5‑x Ga x (R = Gd, Y; x = 1, 1.5, 1.6, 1.7) compounds have been studied. X-ray and electron microprobe analysis show that the samples are single phase and crystallize in the hexagonal CaCu5 - type structure (space group P6/mmm, N 191, hP6). The magnetic properties have been studied from 2 to 400 K under magnetic fields in the region of 1 to 140 kOe. With increasing Ga amount the magnetic ordering temperature decreases rapidly. The increase in Ga concentration leads to the reduction of the magnetic moment of Co sublattice and the Curie temperature. It has been found that the paramagnetic susceptibility follows the Néel-type law for GdCo5‑x Ga x (x = 1.5, 1.6, 1.7) and the Curie-Weiss law for YCo3.3Ga1.7. The molecular field coefficients and sublattice magnetizations were determined on a basis of the Néel theory and experimental data. The magnetocaloric effect and refrigerant capacity have been estimated over a wide temperature range of 10–350 K.

  12. Effect of warming temperatures on US wheat yields

    Science.gov (United States)

    Tack, Jesse; Barkley, Andrew; Nalley, Lawton Lanier

    2015-01-01

    Climate change is expected to increase future temperatures, potentially resulting in reduced crop production in many key production regions. Research quantifying the complex relationship between weather variables and wheat yields is rapidly growing, and recent advances have used a variety of model specifications that differ in how temperature data are included in the statistical yield equation. A unique data set that combines Kansas wheat variety field trial outcomes for 1985–2013 with location-specific weather data is used to analyze the effect of weather on wheat yield using regression analysis. Our results indicate that the effect of temperature exposure varies across the September−May growing season. The largest drivers of yield loss are freezing temperatures in the Fall and extreme heat events in the Spring. We also find that the overall effect of warming on yields is negative, even after accounting for the benefits of reduced exposure to freezing temperatures. Our analysis indicates that there exists a tradeoff between average (mean) yield and ability to resist extreme heat across varieties. More-recently released varieties are less able to resist heat than older lines. Our results also indicate that warming effects would be partially offset by increased rainfall in the Spring. Finally, we find that the method used to construct measures of temperature exposure matters for both the predictive performance of the regression model and the forecasted warming impacts on yields. PMID:25964323

  13. Temperature effects on hospital admissions for kidney morbidity in Taiwan

    International Nuclear Information System (INIS)

    Lin, Yu-Kai; Wang, Yu-Chun; Ho, Tsung-Jung; Lu, Chensheng

    2013-01-01

    Objective: This study aimed to associate hospital admissions of kidney diseases with extreme temperature and prolonged heat/cold events in 7 regions of Taiwan. Methods: Age-specific ( 10 , O 3 , and NO 2 ) and potential confounders. Results: We observed a V or J-shape association between daily average temperatures and the RR estimates for hospital admissions of kidney diseases in Taiwan. The lowest risk for hospital admissions of kidney diseases was found at around 25 °C, and risk increased as temperatures deviated from 25 °C. The pooled cumulative 8-day RR for all ages of population of the 7 study areas were 1.10 (95% confidence interval (CI): 1.01, 1.19) at 18 °C and 1.45 (95% CI: 1.27, 1.64) at 30 °C. High temperature has more profound influence on hospital admission of kidney diseases than low temperature. Temperature risks for hospital admissions were similar between younger (< 65 years) and elderly (65 + years) population. This study observed no significant effects of prolonged heat extremes on hospital admissions of kidney diseases. Conclusions: The heat effect for kidney morbidities leading to hospital admission was more significant than that of the cold temperature. This study did not find the age-dependent relative risks for temperature associating with hospital admissions of kidney diseases. - Highlights: ► V or J-shaped association was observed between daily temperatures and hospital admissions for renal diseases in Taiwan. ► The pooled relative risks accounting for 8 days of lag for the 7 study areas were 1.1 at 18 °C and 1.46 at 30 °C. ► There is no difference of the relative risk estimates for hospital admissions between younger and elderly population. ► We found significant protective effects of hospital admissions for prolonged cold extremes, but not for heat extremes

  14. Load forecasting method considering temperature effect for distribution network

    Directory of Open Access Journals (Sweden)

    Meng Xiao Fang

    2016-01-01

    Full Text Available To improve the accuracy of load forecasting, the temperature factor was introduced into the load forecasting in this paper. This paper analyzed the characteristics of power load variation, and researched the rule of the load with the temperature change. Based on the linear regression analysis, the mathematical model of load forecasting was presented with considering the temperature effect, and the steps of load forecasting were given. Used MATLAB, the temperature regression coefficient was calculated. Using the load forecasting model, the full-day load forecasting and time-sharing load forecasting were carried out. By comparing and analyzing the forecast error, the results showed that the error of time-sharing load forecasting method was small in this paper. The forecasting method is an effective method to improve the accuracy of load forecasting.

  15. Studying the effects of dynamical parameters on reactor core temperature

    Directory of Open Access Journals (Sweden)

    R Khodabakhsh

    2015-01-01

    Full Text Available In order to increase productivity, reduce depreciation, and avoid possible accidents in a system such as fuel rods' melting and overpressure, control of temperature changes in the reactor core is an important factor. There are several methods for solving and analysing the stability of point kinetics equations. In most previous analyses, the effects of various factors on the temperature of the reactor core have been ignored. In this work, the effects of various dynamical parameters on the temperature of the reactor core and stability of the system in the presence of temperature feedback reactivity with external reactivity step, ramp and sinusoidal for six groups of delayed neutrons were studied using the method of Lyapunov exponent. The results proved to be in good agreement with other works

  16. Effects of tissue susceptibility on brain temperature mapping.

    Science.gov (United States)

    Maudsley, Andrew A; Goryawala, Mohammed Z; Sheriff, Sulaiman

    2017-02-01

    A method for mapping of temperature over a large volume of the brain using volumetric proton MR spectroscopic imaging has been implemented and applied to 150 normal subjects. Magnetic susceptibility-induced frequency shifts in gray- and white-matter regions were measured and included as a correction in the temperature mapping calculation. Additional sources of magnetic susceptibility variations of the individual metabolite resonance frequencies were also observed that reflect the cellular-level organization of the brain metabolites, with the most notable differences being attributed to changes of the N-Acetylaspartate resonance frequency that reflect the intra-axonal distribution and orientation of the white-matter tracts with respect to the applied magnetic field. These metabolite-specific susceptibility effects are also shown to change with age. Results indicate no change of apparent brain temperature with age from 18 to 84 years old, with a trend for increased brain temperature throughout the cerebrum in females relative for males on the order of 0.1°C; slightly increased temperatures in the left hemisphere relative to the right; and a lower temperature of 0.3°C in the cerebellum relative to that of cerebral white-matter. This study presents a novel acquisition method for noninvasive measurement of brain temperature that is of potential value for diagnostic purposes and treatment monitoring, while also demonstrating limitations of the measurement due to the confounding effects of tissue susceptibility variations. Copyright © 2016 Elsevier Inc. All rights reserved.

  17. Effects of pressure and temperature on gate valve unwedging

    Energy Technology Data Exchange (ETDEWEB)

    Damerell, P.S.; Harrison, D.H.; Hayes, P.W.; Simons, J.W.; Walker, T.A.

    1996-12-01

    The stem thrust required to unwedge a gate valve is influenced by the pressure and temperature when the valve is closed and by the changes in these conditions between closure and opening. {open_quotes}Pressure locking{close_quotes} and {open_quotes}thermal binding{close_quotes} refer to situations where pressure and temperature effects cause the unwedging load to be much higher than normal. A model of these phenomena has been developed. Wedging (closure) is modeled as developing an {open_quotes}interference{close_quotes} between the disk and its seat rings in the valve. The effects of pressure and temperature are analyzed to determine the change in this disk-to-seat {open_quotes}interference{close_quotes}. Flexibilities, of the disk, body, stem and yoke strongly influence the unwedging thrust. Calculations and limited comparisons to data have been performed for a range of valve designs and scenarios. Pressure changes can increase the unwedging load when there is either a uniform pressure decrease, or a situation where the bonnet pressure exceeds the pressures in the adjacent piping. Temperature changes can increase the unwedging load when: (1) valve closure at elevated system temperature produces a delayed stem expansion, (2) a temperature increase after closure produces a bonnet pressure increase, or (3) a temperature change after closure produces an increase in the disk-to-seat {open_quotes}interference{close_quotes} or disk-to-seat friction.

  18. Effects of pressure and temperature on gate valve unwedging

    International Nuclear Information System (INIS)

    Damerell, P.S.; Harrison, D.H.; Hayes, P.W.; Simons, J.W.; Walker, T.A.

    1996-01-01

    The stem thrust required to unwedge a gate valve is influenced by the pressure and temperature when the valve is closed and by the changes in these conditions between closure and opening. open-quotes Pressure lockingclose quotes and open-quotes thermal bindingclose quotes refer to situations where pressure and temperature effects cause the unwedging load to be much higher than normal. A model of these phenomena has been developed. Wedging (closure) is modeled as developing an open-quotes interferenceclose quotes between the disk and its seat rings in the valve. The effects of pressure and temperature are analyzed to determine the change in this disk-to-seat open-quotes interferenceclose quotes. Flexibilities, of the disk, body, stem and yoke strongly influence the unwedging thrust. Calculations and limited comparisons to data have been performed for a range of valve designs and scenarios. Pressure changes can increase the unwedging load when there is either a uniform pressure decrease, or a situation where the bonnet pressure exceeds the pressures in the adjacent piping. Temperature changes can increase the unwedging load when: (1) valve closure at elevated system temperature produces a delayed stem expansion, (2) a temperature increase after closure produces a bonnet pressure increase, or (3) a temperature change after closure produces an increase in the disk-to-seat open-quotes interferenceclose quotes or disk-to-seat friction

  19. Estimation of abnormal temperature effects on elderly mortality in South Korea using the temperature deviation index

    Science.gov (United States)

    Choi, Giehae; Bae, Hyun-Joo; Lim, Youn-Hee

    2017-07-01

    Recent studies have revealed that the effect of temperature on mortality has changed over time. One of the major contributors to the changes is adaptation. We aimed to understand the relationship between elderly mortality and temperature anomaly using the temperature deviation index (TDI), which considers exposure history. Summertime (May to September) mortality data from 1996 to 2014 and meteorological data from 1971 to 2014 were obtained for 16 regions covering South Korea. The TDI was defined as the target day's temperature abnormality compared to previous 25 years' apparent temperature (AT). The relationship between the TDI and elderly mortality for each region was examined by generalized linear modeling with Poisson distribution. Pooled estimates were computed to yield a national effect estimate. Stratified analyses were performed using the percentiles of AT and TDI. Most regions showed positive linear associations, and the associations ranged from 0.4 to 4.3% increase per unit increase of the TDI. In the pooled analyses, a unit increase of the TDI was associated with a 1.4% increase (95% confidence interval [CI] 0.93-1.87) in elderly mortality. In the stratified analysis, the relationship between the TDI and elderly mortality was significant at or above the 75th percentile of AT (1.32% increase; 95% CI 0.47-2.22). We suggest a positive association between the TDI and elderly mortality in South Korea. The association observed particularly in the highest percentile of AT in the stratified analysis suggests independent effects of temperature anomaly in addition to those of absolute AT.

  20. Estimation of abnormal temperature effects on elderly mortality in South Korea using the temperature deviation index.

    Science.gov (United States)

    Choi, Giehae; Bae, Hyun-Joo; Lim, Youn-Hee

    2017-07-01

    Recent studies have revealed that the effect of temperature on mortality has changed over time. One of the major contributors to the changes is adaptation. We aimed to understand the relationship between elderly mortality and temperature anomaly using the temperature deviation index (TDI), which considers exposure history. Summertime (May to September) mortality data from 1996 to 2014 and meteorological data from 1971 to 2014 were obtained for 16 regions covering South Korea. The TDI was defined as the target day's temperature abnormality compared to previous 25 years' apparent temperature (AT). The relationship between the TDI and elderly mortality for each region was examined by generalized linear modeling with Poisson distribution. Pooled estimates were computed to yield a national effect estimate. Stratified analyses were performed using the percentiles of AT and TDI. Most regions showed positive linear associations, and the associations ranged from 0.4 to 4.3% increase per unit increase of the TDI. In the pooled analyses, a unit increase of the TDI was associated with a 1.4% increase (95% confidence interval [CI] 0.93-1.87) in elderly mortality. In the stratified analysis, the relationship between the TDI and elderly mortality was significant at or above the 75th percentile of AT (1.32% increase; 95% CI 0.47-2.22). We suggest a positive association between the TDI and elderly mortality in South Korea. The association observed particularly in the highest percentile of AT in the stratified analysis suggests independent effects of temperature anomaly in addition to those of absolute AT.

  1. Nuclear Quantum Vibrational Effects in Shock Hugoniot Temperatures

    Energy Technology Data Exchange (ETDEWEB)

    Goldman, N; Reed, E; Fried, L E

    2009-07-23

    We present a straightforward method for the inclusion of quantum nuclear vibrational effects in molecular dynamics calculations of shock Hugoniot temperatures. Using a Grueneisen equation of state and a quasiharmonic approximation to the vibrational energies, we derive a simple, post-processing method for calculation of the quantum corrected Hugoniot temperatures. We have used our novel technique on ab initio simulations of shock compressed water. Our results indicate significantly closer agreement with all available experimental temperature data. Our formalism and technique can be easily applied to a number of different shock compressed molecular liquids or solids.

  2. Temperature effect on Zircaloy-4 stress corrosion cracking

    International Nuclear Information System (INIS)

    Farina, Silvia B.; Duffo, Gustavo S.; Galvele, Jose R.

    1999-01-01

    Stress corrosion cracking (SCC) susceptibility of Zircaloy-4 alloy in chloride, bromide and iodide solutions with variables as applied electrode potential, deformation rate and temperature have been studied. In those three halide solutions the susceptibility to SCC is only observed at potentials close to pitting potential, the crack propagation rate increases with the increase of deformation rate, and that the temperature has a notable effect only for iodide solutions. For chloride and bromide solutions and temperatures ranging between 20 to 90 C degrees it was not found measurable changes in crack propagation rates. (author)

  3. Effect of Chronic Hypercapnia on Body Temperature Regulation

    Science.gov (United States)

    1974-08-01

    temperature in rats at ambient room temperatures of 24 - 28° C. Similar effects have been demon- strated in cats, mice, dogs and rabbits6»7󈨍... glycolysis was found to be reduced 55% during maximal extra- cellular acidosis and showed a partial recovery during the later phase of ex- posure to...as demonstrated by Nahas-and Poyart^T" They observed that adrenalin-induced lipolysis and calorigenesis is inhibited in dogs when breathing a

  4. Effect of increasing growth temperature on yeast fermentation ...

    African Journals Online (AJOL)

    The effect of increasing growth temperature on yeast fermentation was studied at approximately 5 oC intervals over a range of 18 – 37 oC, using one strain each of ale, lager and wine yeast. The ale and wine yeasts grew at all the temperatures tested, but lager yeast failed to grow at 37 oC. All these strains gave lower ...

  5. Temperature effects on surface activity and application in oxidation ...

    Indian Academy of Sciences (India)

    Keywords. Surface activity; cetyl trimethylammonium bromide; sodium dodecyl sulfate; temperature; oxidation. ... Catalytic effect on oxidation of toluene derivatives with potassium permanganate follows the order CTAB-SDS > SDS > CTAB. This is not caused by the dissociative effect of CTAB-SDS with low surface activity at ...

  6. H/D isotope effects in high temperature proton conductors

    NARCIS (Netherlands)

    Bonanos, N.; Huijser, Jannetje Maria; Poulsen, F.W.

    2015-01-01

    The atomic mass ratio of ca. 2 between deuterium and hydrogen is the highest for any pair of stable isotopes and results in significant and measurable H/D isotope effects in high temperature proton conductors containing these species. This paper discusses H/D isotope effects manifested in O–H/O–D

  7. Temperature effects on the hydrophobic force between two ...

    Indian Academy of Sciences (India)

    TUHIN SAMANTA

    2018-03-02

    Mar 2, 2018 ... Abstract. Water-mediated, effective, long-range interaction between two hydrophobic surfaces immersed in water is of great importance in natural phenomena. We perform the molecular dynamics simulations to investigate the effect of temperature on the attractive force between two graphene-like ...

  8. Effect of Pyrolysis Temperature on Cadmium and Lead ...

    African Journals Online (AJOL)

    Consumption of tobacco as cigarette or otherwise has been demonstrated to contribute to air pollution via smoke generation resulting in adverse health effect. Therefore, this study investigates the effect of pyrolysis temperature on the concentration, distribution of cadmium and lead between ash residue and smoke in some ...

  9. A comparison between rare earth and transition metals working as magnetic materials in an AMR refrigerator in the room temperature range

    International Nuclear Information System (INIS)

    Aprea, C.; Greco, A.; Maiorino, A.; Masselli, C.

    2015-01-01

    This paper describes a two-dimensional (2D) multiphysics model of a packed bed regenerator made of magnetocaloric material. The regenerator operates as a refrigerant for a magnetic refrigerator operating at room temperature on the strength of an active magnetic regenerator (AMR) cycle. The model is able to simulate the thermofluidodynamic behavior of the magnetocaloric material and the magnetocaloric effect of the refrigerant. The model has been validated by means of experimental results. Different magnetic materials have been tested with the model as refrigerants: pure gadolinium, second order phase magnetic transition Pr 0.45 Sr 0.35 MnO 3 and first order phase magnetic transition alloys Gd 5 (Si x Ge 1−x ) 4 , LaFe 11.384 Mn 0.356 Si 1.26 H 1.52 , LaFe 11.05 Co 0.94 Si 1.10 and MnFeP 0.45 As 0.55 . The tests were performed with fixed fluid flow rate (5 l/min), AMR cycle frequency (1.25 Hz) and cold heat exchanger temperature (288 K) while the hot heat exchanger temperature was varied in the range 295–302 K. The results, generated for a magnetic induction which varies from 0 to 1.5 T, are presented in terms of temperature span, refrigeration power and coefficient of performance. From a global point of view (performances and cost), the most promising materials are LaFeSi compounds which are really cheaper than rare earth compounds and they give a performance sufficiently higher than gadolinium. - Graphical abstract: • Active Magnetic Refrigeration (AMR) cycle; • First Order Transition magnetic materials (FOMT); • Second Order Transition magnetic materials (SOMT). - Highlights: • Comparison between different magnetic materials. • 2D model of an Active Magnetic Regenerative refrigeration cycle. • Validation of the model with experimental data. • Gd 5 (Si x Ge 1−x ) 4 is the most performant magnetic material. • The most promising are LaFeSi compounds which are cheaper and they give high performances.

  10. Magnetic refrigeration--towards room-temperature applications

    International Nuclear Information System (INIS)

    Brueck, E.; Tegus, O.; Li, X.W.; Boer, F.R. de; Buschow, K.H.J.

    2003-01-01

    Modern society relies very much on readily available cooling. Magnetic refrigeration based on the magneto-caloric effect (MCE) has become a promising competitive technology for the conventional gas-compression/expansion technique in use today. Recently, there have been two breakthroughs in magnetic-refrigeration research: one is that American scientists demonstrated the world's first room-temperature, permanent-magnet, magnetic refrigerator; the other one is that we discovered a new class of magnetic refrigerant materials for room-temperature applications. The new materials are manganese-iron-phosphorus-arsenic (MnFe(P,As)) compounds. This new material has important advantages over existing magnetic coolants: it exhibits a huge MCE, which is larger than that of Gd metal; and its operating temperature can be tuned from about 150 to about 335 K by adjusting the P/As ratio. Here we report on further improvement of the materials by increasing the Mn content. The large entropy change is attributed to a field-induced first-order phase transition enhancing the effect of the applied magnetic field. Addition of Mn reduces the thermal hysteresis, which is intrinsic to the first-order transition. This implies that already moderate applied magnetic fields of below 2 T may suffice

  11. Canceling effect leads temperature insensitivity of hydrolytic enzymes in soil

    Science.gov (United States)

    Razavi, Bahar S.; Blagodatskaya, Evgenia; Kuzyakov, Yakov

    2015-04-01

    Extracellular enzymes are important for decomposition of many macromolecules abundant in soil such as cellulose, hemicelluloses and proteins (Allison et al., 2010; Chen et al., 2012). The temperature sensitivity of enzymes responsible for organic matter decomposition is the most crucial parameter for prediction of the effects of global warming on carbon cycle. Temperature responses of biological systems are often expressed as a Q10 functions; The Q10 describes how the rate of a chemical reaction changes with a temperature increase for 10 °C The aim of this study was to test how the canceling effect will change with variation in temperature interval, during short-term incubation. We additionally investigated, whether canceling effect occurs in a broad range of concentrations (low to high) and whether it is similar for the set of hydrolytic enzymes within broad range of temperatures. To this end, we performed soil incubation over a temperature range of 0-40°C (with 5°C steps). We determined the activities of three enzymes involved in plant residue decomposition: β-glucosidase and cellobiohydrolase, which are commonly measured as enzymes responsible for degrading cellulose (Chen et al., 2012), and xylanase, which degrades xylooligosaccharides (short xylene chain) in to xylose, thus being responsible for breaking down hemicelluloses (German et al., 2011). Michaelis-Menten kinetics measured at each temperature allowed to calculate Q10 values not only for the whole reaction rates, but specifically for maximal reaction rate (Vmax) and substrate affinity (Km). Subsequently, the canceling effect - simultaneous increase of Vmax and Km with temperature was analyzed within 10 and 5 degree of temperature increase. Three temperature ranges (below 10, between 15 and 25, and above 30 °C) clearly showed non-linear but stepwise increase of temperature sensitivity of all three enzymes and allowed to conclude for predominance of psychrophilic, mesophilic and thermophilic

  12. Theoretical investigations on the magnetocaloric and electrical properties of a perovskite manganite La(0.67)Ba(0.1)Ca(0.23)MnO3.

    Science.gov (United States)

    Abassi, Mounira; Mohamed, Za; Dhahri, J; Hlil, E K

    2016-03-21

    An investigation of the magnetic, magnetocaloric and electrical behavior of La(0.67)Ba(0.1)Ca(0.23)MnO3 is presented. The variation of magnetization (M) vs. temperature (T) under 1, 2, 3, 4 and 5 T magnetic fields reveals a ferromagnetic-paramagnetic transition. Magnetic entropy change, relative cooling power and specific heat for magnetic field variation were conducted using a phenomenological model. Moreover, the electrical resistivity is fitted with the phenomenological percolation model which is based on the phase segregation of ferromagnetic metallic clusters and paramagnetic insulating regions. The equation of the form ΔS(P)(M)(T,H) = - α∫(H)(0)[∂(ln)(ρ)/∂(T)](H)(dH) relates the magnetic order to the transport behavior of our sample. The results show that the as obtained magnetic entropy change values are similar to those determined using data obtained from the investigation of the dependence of magnetization on the temperature and magnetic field.

  13. Temperature, humidity and time., Combined effects on radiochromic film dosimeters

    International Nuclear Information System (INIS)

    Abdel-Fattah, A.A.; Miller, A.

    1996-01-01

    The effects of both relative humidity and temperature during irradiation on the dose response of FWT-60-00 and Riso B3 radiochromic film dosimeters have been investigated in the relative humidity (RH) range 11-94% and temperature range 20-60 o C for irradiation by 60 Co photons and 10-MeV electrons. The results show that humidity and temperature cannot be treated as independent variables, rather there appears to be interdependence between absorbed dose, temperature, and humidity. Dose rate does not seem to play a significant role. The dependence of temperature during irradiation is + 0.25 ± 0.1% per o C for the FWT-60-00 dosimeters and +0.5 ± 0.1% per o C for Riso B3 dosimeters at temperatures between 20 and 50 o C and at relative humidities between 20 and 53%. At extreme conditions both with respect to temperature and to humidity, the dosimeters show much stronger dependences. Whenever possible one should use dosimeters sealed in pouches under controlled intermediate humidity conditions (30-50%) or, if that is impractical, one should maintain conditions of calibration as close as possible to the conditions of use. Without that precaution, severe dosimetry errors may result. (author)

  14. Temperature effect on vortex-core reversals in magnetic nanodots

    Science.gov (United States)

    Kim, Bosung; Yoo, Myoung-Woo; Lee, Jehyun; Kim, Sang-Koog

    2015-05-01

    We studied the temperature effect on vortex-core reversals in soft magnetic nanodots by micromagnetic numerical calculations within a framework of the stochastic Landau-Lifshitz-Gilbert scheme. It was determined that vortex-core-switching events at non-zero temperatures occur stochastically, and that the threshold field strength increases with temperature for a given field frequency. The mechanism of core reversals at elevated temperatures is the same as that of vortex-antivortex-pair-mediated core reversals found at the zero temperature. The reversal criterion is also the out-of-plane component of a magnetization dip that should reach -p, which is to say, m z , dip = -p, where p is the original polarization, p = +1 (-1), for the upward (downward) core. By this criterion, the creation of a vortex-antivortex pair accompanies complete vortex-antivortex-annihilation-mediated core reversals, resulting in the maximum excess of the exchange energy density, Δ Eex cri ≈ 15.4 ± 0.2 mJ/cm3. This work provides the underlying physics of vortex-core reversals at non-zero temperatures, and potentiates the real application of vortex random access memory operating at elevated temperatures.

  15. Effect of temperature to the properties of sago starch

    Science.gov (United States)

    Mustafa Kamal, M.; Baini, R.; Mohamaddan, S.; Selaman, O. S.; Zauzi, N. Ahmad; Rahman, M. R.; Rahman, N. Abdul; Chong, K. H.; Atan, M. F.; Samat, N. A. S. Abdul; Taib, S. N. L.; Othman, A. K.

    2017-06-01

    Recently, the importance of sago starch has increased, as it has become one of the main economically important agricultural crops to the most Southeast Asia countries. In the present work, an analysis on drying process of sago starch (Metroxylon sagu Rottb.) underwent various temperature has been made by using four empirical equations. The main goal of this analysis is to suggest the most accurate equation, in order to model and simulate the mechanical drying of sago starch. The experimental investigations were carried out in a gravity convection lab oven; and ±50g of sago starch (sample heights of 1 cm) was dried through four different temperatures, which were 50, 60, 70 and 80ºC. The effect of drying temperature on the drying kinetics, as well as various qualities attributes of sago starch, such as microstructure, colour and functional properties were investigated. The results suggested that drying temperature has significant effect on sago starch drying kinetic; therefore, drying temperature would be the basis to select drying condition. Meanwhile, it was found that the various drying temperature ranging from 50 to 80ºC affected the product quality especially in term of colour.

  16. Temperature effects on interaction of positive ions with plastic detectors

    International Nuclear Information System (INIS)

    Mendoza Anaya, D.

    1992-01-01

    The range of heavy charged particles in matter is dependent mainly on two groups of parameters, one related to the particle characteristics (charge z, mass m, energy E) and the other characterized by the stopping medium (charge z, density ρ). Those two groups are enough to describe the particle energy lost, which is related to the residual range. Research on charge particles registration using solid state nuclear track detectors (SSNTD), probe that environmental parameters affect the stabilization and formation of the tracks. One of those, is the temperature detector which shows an important effect during the irradiation on the characteristics of the tracks produced. In order to study the dependence of track geometry as a function of irradiation temperature, some SSNTD (CR 39 type) were irradiated with α particles and fission fragments. Results of this work show the existence of irradiation temperature effect on the track geometry. It is observed a reduction of length and diameters, as temperature increases. For low irradiation temperatures, there is a reduction of the track geometry, as compared with environmental temperature. (Author)

  17. Effects of MDMA on body temperature in humans

    Science.gov (United States)

    Liechti, Matthias E

    2014-01-01

    Hyperthermia is a severe complication associated with the recreational use of 3,4-methylenedioxymethamphetamine (MDMA, Ecstasy). In this review, the clinical laboratory studies that tested the effects of MDMA on body temperature are summarized. The mechanisms that underlie the hyperthermic effects of MDMA in humans and treatment of severe hyperthermia are presented. The data show that MDMA produces an acute and dose-dependent rise in core body temperature in healthy subjects. The increase in body temperature is in the range of 0.2-0.8°C and does not result in hyperpyrexia (>40°C) in a controlled laboratory setting. However, moderately hyperthermic body temperatures >38.0°C occur frequently at higher doses, even in the absence of physical activity and at room temperature. MDMA primarily releases serotonin and norepinephrine. Mechanistic clinical studies indicate that the MDMA-induced elevations in body temperature in humans partially depend on the MDMA-induced release of norepinephrine and involve enhanced metabolic heat generation and cutaneous vasoconstriction, resulting in impaired heat dissipation. The mediating role of serotonin is unclear. The management of sympathomimetic toxicity and associated hyperthermia mainly includes sedation with benzodiazepines and intravenous fluid replacement. Severe hyperthermia should primarily be treated with additional cooling and mechanical ventilation. PMID:27626046

  18. Remote sensing of land surface temperature: The directional viewing effect

    International Nuclear Information System (INIS)

    Smith, J.A.; Schmugge, T.J.; Ballard, J.R. Jr.

    1997-01-01

    Land Surface Temperature (LST) is an important parameter in understanding global environmental change because it controls many of the underlying processes in the energy budget at the surface and heat and water transport between the surface and the atmosphere. The measurement of LST at a variety of spatial and temporal scales and extension to global coverage requires remote sensing means to achieve these goals. Land surface temperature and emissivity products are currently being derived from satellite and aircraft remote sensing data using a variety of techniques to correct for atmospheric effects. Implicit in the commonly employed approaches is the assumption of isotropy in directional thermal infrared exitance. The theoretical analyses indicate angular variations in apparent infrared temperature will typically yield land surface temperature errors ranging from 1 to 4 C unless corrective measures are applied

  19. Temperature effects on the blood oxygen affinity in sharks.

    Science.gov (United States)

    Bernal, Diego; Reid, Joseph P; Roessig, Julie M; Matsumoto, Shinsyu; Sepulveda, Chugey A; Cech, Joseph J; Graham, Jeffrey B

    2018-03-05

    In fish, regional endothermy (i.e., the capacity to significantly elevate tissue temperatures above ambient via vascular heat exchangers) in the red swimming muscles (RM) has evolved only in a few marine groups (e.g., sharks: Lamnidae, Alopiidae, and teleosts Scombridae). Within these taxa, several species have also been shown to share similar physiological adaptations to enhance oxygen delivery to the working tissues. Although the hemoglobin (Hb) of most fish has a decreased affinity for oxygen with an increase in temperature, some regionally endothermic teleosts (e.g., tunas) have evolved Hbs that have a very low or even an increased affinity for oxygen with an increase in temperature. For sharks, however, blood oxygen affinities remain largely unknown. We examined the effects of temperature on the blood oxygen affinity in two pelagic species (the regionally endothermic shortfin mako shark and the ectothermic blue shark) at 15, 20, and 25 °C, and two coastal ectothermic species (the leopard shark and brown smooth-hound shark) at 10, 15, and 20 °C. Relative to the effects of temperature on the blood oxygen affinity of ectothermic sharks (e.g., blue shark), shortfin mako shark blood was less affected by an increase in temperature, a scenario similar to that documented in some of the tunas. In the shortfin mako shark, this may act to prevent premature oxygen dissociation from Hb as the blood is warmed during its passage through vascular heat exchangers. Even though the shortfin mako shark and blue shark occupy a similar niche, the effects of temperature on blood oxygen affinity in the latter more closely resembled that of the blood in the two coastal shark species examined in this study. The only exception was a small, reverse temperature effect (an increase in blood oxygen affinity with temperature) observed during the warming of the leopard shark blood under simulated arterial conditions, a finding that is likely related to the estuarine ecology of this

  20. Temperature effect on 4-aminophtalimide fluorescence in n-alcohols

    Energy Technology Data Exchange (ETDEWEB)

    Dobek, Krzysztof, E-mail: dobas@amu.edu.pl [Faculty of Physics, Adam Mickiewicz University, Umultowska 85, 61-614 Poznan (Poland); Karolczak, Jerzy, E-mail: jgkarol@amu.edu.pl [Faculty of Physics, Adam Mickiewicz University, Umultowska 85, 61-614 Poznan (Poland); Center For Ultrafast Laser Spectroscopy, Adam Mickiewicz University, Umultowska 85, 61-614 Poznan (Poland)

    2015-09-15

    The compound 4-aminophthalimide (4-AP) is a well-known dye used as an environment polarity sensitive probe e.g. in solvation studies. This paper presents the effect of temperature on 4-aminophthalimides steady-state and time-resolved fluorescence in five n-alcohols. It is shown that the hydrogen bonding ability of n-alcohols affects the shifts of steady-state absorption and fluorescence spectra of 4-aminophthalimide at room temperature, and the shifts of fluorescence also at temperatures from the range 180 to 323 K. Temperature is shown to affect the change in hydrogen bond energy that follows 4-AP excitation, in a way dependent on the n-alcohol alkyl chain length. On the other hand, time-resolved results indicate that the temperature dependence of 4-AP deactivation follows mainly from the energy-gap dependent non-radiative deactivation rate. Fluorescence transition dipole moments at room temperature have been found to be slightly dependent on the solvent, but nothing proves that these changes are connected to different hydrogen bonding character of each n-alcohol. Therefore, while the steady-state results provide clear evidence of hydrogen bonding between 4-AP and n-alcohols, the time-resolved results do not show any evident sign of hydrogen bonding, besides the influence of the position of fluorescence emission on the radiative and non-radiative rates. - Highlights: • We show temperature effect on 4-aminophthalimide (4-AP) absorption and emission. • Hydrogen bonds formation between n-alcohols and 4-AP affect steady-state results. • Temperature change influences hydrogen bonds energy. • 4-AP non-radiative deactivation is energy-gap controlled.