Investigating the magnetic entropy change in single-phase Y2Fe17 melt-spun ribbons

"The inspection of simplified fabrication and/or processing routes in order to produce materials with attractive magnetocaloric properties is of paramount importance for the development of environmentally friendly magnetic cooling technology. In this work, we have made use of the melt-spinning...

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Detalles Bibliográficos
Autores: JOSE LUIS SANCHEZ LLAMAZARES, Pablo Álvarez Alonso, CESAR FIDEL SANCHEZ VALDES, Pablos Jesús Ibarra Gaytán, Jesús Angel Blanco Rodríguez, Pedro Gorria
Tipo de recurso: artículo
Estado:Versión aceptada para publicación
Fecha de publicación:2016
País:México
Institución:Instituto Potosino de Investigación Científica y Tecnológica
Repositorio:Repositorio Institucional del IPICYT
OAI Identifier:oai:ipicyt.repositorioinstitucional.mx:1010/1935
Acceso en línea:http://ipicyt.repositorioinstitucional.mx/jspui/handle/1010/1935
Access Level:acceso abierto
Palabra clave:info:eu-repo/classification/Autor/Y2Fe17 intermetallics
info:eu-repo/classification/Autor/Melt-spun ribbons
info:eu-repo/classification/Autor/Magnetocaloric effect
info:eu-repo/classification/Autor/Magnetic entropy change
info:eu-repo/classification/Autor/Refrigerant capacity
info:eu-repo/classification/cti/1
info:eu-repo/classification/cti/22
Descripción
Sumario:"The inspection of simplified fabrication and/or processing routes in order to produce materials with attractive magnetocaloric properties is of paramount importance for the development of environmentally friendly magnetic cooling technology. In this work, we have made use of the melt-spinning technique to obtain directly single-phase Y2Fe17 polycrystalline ribbons avoiding any high-temperature annealing for phase consolidation and homogenization. The melt-spun ribbons, with hexagonal Th2Ni17-type crystal structure, exhibit a moderate maximum value of the magnetic entropy change, |?SMpeak| = 2.4(4.4) J kg?1 K?1 under an applied magnetic field change of 2(5) T. Although these values are similar to those for the bulk alloy, the ?SM(T) curves are manifestly broader, thus giving rise to an expansion of the working temperature range and the enhancement of about 15% in the refrigerant capacity. We also show that the magnetic field dependence of |?SMpeak| at T = TC follows a H2/3 power-law."