Large magnetic entropy change and magnetic phase transitions in rapidly quenched bulk Mn-Fe-P-Si alloys
Mn1.15Fe0.85P0.50Si0.45B0.05 alloys were prepared by copper mold suction casting method. Subsequent annealing processes were employed to tune the microstructures and magnetocaloric effects. Results show that Mn1.15Fe0.85P0.50Si0.45B0.05 alloys crystallize in a hexagonal phase with the Fe2P structure...
Gespeichert in:
Veröffentlicht in: | Journal of alloys and compounds 2017-11, Vol.725, p.1069-1076 |
---|---|
Hauptverfasser: | , , , , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | Mn1.15Fe0.85P0.50Si0.45B0.05 alloys were prepared by copper mold suction casting method. Subsequent annealing processes were employed to tune the microstructures and magnetocaloric effects. Results show that Mn1.15Fe0.85P0.50Si0.45B0.05 alloys crystallize in a hexagonal phase with the Fe2P structure type. With increasing annealing temperature, the lattice parameters of a and c of Fe2P-type phase increase from 5.7988(1)Å to 6.0785(2)Å and from 3.3218(1)Å to 3.4727(2)Å for the Mn1.15Fe0.85P0.50Si0.45B0.05 alloys according to XRD. At the same time the Curie temperature and magnetic entropy change increase from 233 K to 244 K and from 8.8 J kg−1K−1 to 17.0 J kg−1K−1 (ΔH = 2 T), respectively, while the thermal hysteresis decreases. The entropy changes of these alloys are also estimated from the Clausius-Clapeyron equation, Landau theory and heat capacity, respectively. The nature of the phase transitions were studied through the Arrott plots, which indicate that the samples undergo first-order ferro-paramagnetic phase transitions. However, the universal curve of scaled magnetic entropy change reveals that during the magnetic phase transition, there exists a critical magnetic field, about 1.25 T, below which the sample undergoes a second-order phase transition and above which it displays a first-order phase transition. Furthermore, mechanisms for the large magnetic entropy change and possibilities for the room-temperature magnetic refrigeration are discussed.
•Mn1.15Fe0.85P0.5Si0.45B0.05 alloy was prepared by copper mold suction casting method.•Tc and −ΔS can be tuned by heat treatment temperature.•−ΔS are evaluated by Maxwell, C-C equation, Landau theory and heat capacity from DSC.•The first order phase transition is induced by magnetic and temperature fields. |
---|---|
ISSN: | 0925-8388 1873-4669 |
DOI: | 10.1016/j.jallcom.2017.07.243 |