M. Solzi, G. Porcari, F. Cugini DiFeST - Dipartimento di Fisica e Scienze della Terra Università di Parma, Italy Dynamic response of magnetocaloric materials.

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M. Solzi, G. Porcari, F. Cugini DiFeST - Dipartimento di Fisica e Scienze della Terra Università di Parma, Italy Dynamic response of magnetocaloric materials

DiFeST Università di Parma Energy and environment 2 General problem of energy conversion Refrigeration: food conservation, household appliances 25% of residential and 15% of commercial power consumption Constraints: Montreal (1987), Kyoto (1997) protocols Present technologies: vapour compression cycles with ozone depleting gases (CFCs, HCFCs) greenhouse gases (CFCs, HCFCs, HFC)

DiFeST Università di Parma A promising alternative: a green technology 3 Energy conversion (cooling) based on the magnetocaloric effect near RT: No harmful gases involved, low pressure Compactness (solid-state materials), low noise Better efficiency? Maybe 60% theor. limit «nearly-commercial» prototypes K. Engelbrecht, et al., Int. J. Refrig. 2012

DiFeST Università di Parma The MagnetoCaloric Effect 4 Heat absorbed Heat released Temperature, T Entropy, S S(HB)S(HB) S(HA)S(HA) H B >H A  T ad (T,  H) TB(HB)TB(HB) ST(T,H)ST(T,H) SB(HB)SB(HB) SA,TASA,TA TcTc MCE Temperature, T

DiFeST Università di Parma Magnetocaloric materials 5 «Classic» materials: Gd  reference Curie transition «Giant» MC materials: Magneto-structural Magneto-structural transitions 1 st -order transitions 1 st -order transitions Example of recent promising materials: |  T ad | (K) T c, T m (K) Gd LCSMO (1) MnFePSiB (5) LaFeSiH (4) Gd 5 Si 2 Ge 2 (3) NiMnIn-Co (2) Best reversible |  T ad | in 1 T (1)Ch. Bahl, et al., Appl. Phys. Lett (2)T. Gottschall, et al. Appl. Phys. Lett (3)L. von Moos, J. Phys. D Appl. Phys (4)J. Lyubina, Adv. Mater (5)F. Guillou, et al., J. Appl. Phys. 2014

DiFeST Università di Parma The end of the story? 6 Good materials and working devices: thus are we at the end of the story? No, there are many open questions: Materials: Hysteresis Hysteresis of 1 st order transitions Reproducibility Reproducibility of thermomagnetic properties Thermal conductivity, mechanical stability, … Devices: Lower efficiency and power/temperature span, higher costs  still promising but not imminent commercial applicability! J. Steven Brown, P.A. Domanski, Applied Thermal Engineering 64, 252 (2014)

DiFeST Università di Parma Characterization of the Magnetocaloric effect “conventional” techniques: Indirect Indirect:  S T (T,  H) from magnetization curves 7 Ni 45 Co 5 Mn 32 Ga 8 Measurement protocol: L. Caron, et al.,J. Magn. Magn. Mater. 321, 3559 (2009)

DiFeST Università di Parma Characterization of the Magnetocaloric effect “conventional” techniques: Indirect Indirect:  S T (T,  H) from magnetization curves  S T (T,  H) and  T ad (T,  H) from magnetic Differential Scanning Calorimetry 8 Model: S. Jeppesen, et al., Rev. Sci. Instrum. 79, (2008) V. Basso, et al., Rev. Sci. Instrum. 81, (2010)  0 H = 1.8 T  0 H = 0  0 H = 1.8 T  0 H = 0 Ni 45 Co 5 Mn 32 Ga 8

DiFeST Università di Parma Characterization of the Magnetocaloric effect “conventional” techniques: Indirect Indirect:  S T (T,  H) from magnetization curves  S T (T,  H) and  T ad (T,  H) from magnetic Differential Scanning Calorimetry Direct Direct:  T ad (T,  H) from adiabatic temperature change measurements 9 G. Porcari et al., Rev. Sci. Instrum., 84, (2013) Gd

DiFeST Università di Parma Characterization of the Magnetocaloric effect “conventional” techniques: Indirect Indirect:  S T (T,  H) from magnetization curves  S T (T,  H) and  T ad (T,  H) from magnetic Differential Scanning Calorimetry Direct Direct:  T ad (T,  H) from adiabatic temperature change measurements Reproducibility Reproducibility of meas. for different samples (1 st order transitions) mass, shape, micro-strains, composition … comparison Importance of comparison of different techniques 10 V. K. Pecharsky and K. A. Gschneidner, Jr, J. Appl. Phys., 90, 4614 (2001)

DiFeST Università di Parma Iso-thermal entropy change: comparison 11 G. Porcari et al., Phys. Rev. B, 86, (2012) Ni 45 Co 5 Mn 32 Ga 8

DiFeST Università di Parma Adiabatic temperature change: comparison G. Porcari et al., Phys. Rev. B, 86, (2012) G. Porcari et al., Phys. Rev. B, 85, (2012) 12  0 d H /d t = 2 T/s  0 d H /d t = 10  3 T/s Ni 45 Co 5 Mn 32 Ga 8

DiFeST Università di Parma Thermomagnetic cycles 13 operating (dynamic) conditions Study of MCE in operating (dynamic) conditions cycles Repeated thermomagnetic cycles G. Porcari, et al., Rev. Sci. Instrum. 84, (2013) Pneumatic linear actuator Two regions with controlled H and T

DiFeST Università di Parma Thermomagnetic cycles 14 G. Porcari, et al., Rev. Sci. Instrum. 84, (2013) Gd polycrystalline sample

DiFeST Università di Parma Time constant of temperature change 15 thermal conductivity Comparison of materials with different thermal conductivity: composites Different magnitude of the effect and different frequency LCMO - k= 1.3 Wm -1 K -1 LCMO-Ag filled – k= 2.2 Wm -1 K -1 G. Porcari, et al., Int. J. Refrig., in press (2015)

DiFeST Università di Parma Time constant of temperature change 16 Time decay Time decay of the adiabatic branch: time constant  Exponential best fit + average on hundreds of cycles Heat-transfer simulations (FEM) G. Porcari, et al., Int. J. Refrig., in press (2015)

DiFeST Università di Parma Time constant of temperature change 17 dynamic response  represents the dynamic response of a MC material Upper bound for max operating frequency microstructure Indirect information on the microstructure evolution with N. of cycles mechanical stability  thermal conductivity G. Porcari, et al., Int. J. Refrig., in press (2015) experimental FEM simulations

DiFeST Università di Parma Non-contact measurements techniques 18 non-contact techniques Direct methods for measuring  T ad based on non-contact techniques: nearly-ideal adiabatic conditions; thermomagnetic cycles at relatively high frequency (  10 Hz); samples with reduced thickness, like as thin sheets and ribbons (  thin films) Acoustic or optical detection of thermal radiation (low ac magnetic fields) A. O. Guimarães, et al., Phys. Rev. B 80, (2009) J. Döntgen, et al., Appl. Phys. Lett. 106, (2015)

DiFeST Università di Parma Non-contact techniques: an example 19 F. Cugini, et al., Rev. Sci. Instrum. 85, (2014)

DiFeST Università di Parma Non-contact techniques: experiments 20  0  H = 2 T Gd bulk F. Cugini, et al., Rev. Sci. Instrum. 85, (2014) Gd sheets Heat transfer simulations + experiments Validation

DiFeST Università di Parma Non-contact techniques: time scale of H change 21  magn (s) Thermopile limit F. Cugini, et al., Rev. Sci. Instrum. 85, (2014) Magnetic field time constant Detectable fraction of  T ad Gd sheets -  0  H = 1.0 T electromagnet switch on/off 100 %

Thermal lensing (mirage effect) 22

Non-contact techniques: thermal lensing 23 laser coil sample Pt100 heater detector Pulsed magnetic field F. Cugini, et al., submitted to Appl. Phys. Lett. (2015)

Non-contact techniques: thermal lensing 24 Fast response time: < ms agreement with usual techniques for measuring Δ T ad Bulk MnFeP 45 As 55 F. Cugini, et al., submitted to Appl. Phys. Lett. (2015)

DiFeST Università di Parma Conclusions 25 Comparison of different techniques for characterization of MC refrigerants Nearly operating conditions: repeated cycles Dynamic response: time constant of temperature change Non-contact measurements: high frequency – low mass materials Comparison of experimental data with heat transfer simulations

DiFeST Università di Parma Acknowledgments 26 F. Albertini, S. Fabbrici F. Albertini, S. Fabbrici Istituto IMEM-CNR, Parma, Italy E. Brück, L. Caron, F. Guillou, N.H. van Dijk E. Brück, L. Caron, F. Guillou, N.H. van Dijk FAME, Technical University of Delft (the Netherlands) L. Cohen, K. Morrison, J. Turcaud L. Cohen, K. Morrison, J. Turcaud Blackett Laboratory, Imperial College, London (UK) Loughborough University (UK) C. Felser C. Felser Max-Planck-Institut für Chemische Physik fester Stoffe, Dresden (Germany)