dc.contributorAmerican Institute of Physics
dc.creatorSánchez Llamazares, José Luis
dc.creatorFlores Zúñiga, Horacio
dc.creatorSánchez Valdés, Cesar Fidel
dc.creatorC. A. Ross
dc.creatorCarlos Garcia
dc.date2018-04-03T19:23:07Z
dc.date2018-04-03T19:23:07Z
dc.date2012-04
dc.date.accessioned2023-07-17T22:04:10Z
dc.date.available2023-07-17T22:04:10Z
dc.identifierJ. L. Sánchez Llamazares et al., Journal of Applied Physics 111, 07A932 (2012); https://doi.org/10.1063/1.3676606
dc.identifierhttp://hdl.handle.net/11627/3766
dc.identifierhttps://doi.org/10.1063/1.3676606
dc.identifier.urihttps://repositorioslatinoamericanos.uchile.cl/handle/2250/7543848
dc.description"The thermal dependence of the magnetic entropy change (Delta S-M(T)) and refrigerant capacity (RC) of austenite in as-quenched ribbons of chemical composition Ni51.1Mn31.2In17.7 produced by melt spinning at a high cooling rate of 48 ms(-1) is reported. The effect of annealing at 1073 K on the structure and the magnetic properties was studied. The as-quenched sample is a single-phase austenite that presents a B2 ordered structure. The annealing on the melt spun samples produced a L2(1)-type ordered structure. Austenite is characterized by a broad Delta S-M(T) curve that, for a field change of 5.0 T, exhibits a full-width at half-maximum delta T-FMHW of 107 K, a peak value of the magnetic entropy change Delta S-M(peak) of -3.1 Jkg(-1) K-1, and RC = 345 Jkg(-1). Although annealed samples show larger Delta S-M(peak) values the narrower Delta S-M(T) curves leads to a reduction in RC. Thus, the as-quenched sample shows a higher efficiency for a refrigerant cycle."
dc.formatapplication/pdf
dc.rightsAttribution-NonCommercial-NoDerivatives 4.0 Internacional
dc.rightshttp://creativecommons.org/licenses/by-nc-nd/4.0/
dc.rightsAcceso Abierto
dc.subjectFÍSICA
dc.titleRefrigerant capacity of austenite in as-quenched and annealed Ni51.1Mn31.2In17.7 melt spun ribbons
dc.typearticle


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