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Magnetic entropy change and refrigerant capacity of rapidly solidified TbNi2 alloy ribbons

dc.contributor.authorSánchez Llamazares, José Luis
dc.contributor.authorSánchez Valdés, Cesar Fidel
dc.contributor.authorIbarra Gaytán, Pablo Jesús
dc.contributor.authorÁlvarez Alonso, Pablo
dc.contributor.authorGorria, Pedro
dc.contributor.authorBlanco Rodríguez, Jesús Angel
dc.contributor.editorAmerican Institute of Physics
dc.date.accessioned2018-04-03T19:23:09Z
dc.date.available2018-04-03T19:23:09Z
dc.date.issued2013-05
dc.identifier.citationJ. L. Sánchez Llamazares et al., Journal of Applied Physics 113, 17A912 (2013); https://doi.org/10.1063/1.4794988
dc.identifier.urihttp://hdl.handle.net/11627/3769
dc.description.abstract"The magnetocaloric effect in TbNi2 alloy ribbons synthesized by rapid solidification was investigated. This material crystallizes in a superstructure of the cubic Laves phase structure type C15 (space group F-43m). The saturation magnetization and Curie temperature are M-S = 134 +/- 2A m(2) kg(-1) and T-C = 37 +/- 1K, respectively. For a magnetic field change of 5 T, the material shows a maximum magnetic entropy change vertical bar Delta S-M(peak)vertical bar = 13.9 J kg(-1) K-1, with a full-width at half-maximum delta T-FWHM = 32 K, and a refrigerant capacity RC = 441 J kg(-1). The RC value is similar to those reported for other magnetic refrigerants operating within the temperature range of 10-80 K. Finally, it is worth noting that the use of rapid solidification circumvents the necessity for longterm high-temperature homogenization processes normally needed with these RNi2 alloys."
dc.rightsAttribution-NonCommercial-NoDerivatives 4.0 Internacional
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/4.0/
dc.subject.classificationFÍSICA
dc.titleMagnetic entropy change and refrigerant capacity of rapidly solidified TbNi2 alloy ribbons
dc.typearticle
dc.identifier.doihttps://doi.org/10.1063/1.4794988
dc.rights.accessAcceso Abierto


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