Phase transformation and magnetocaloric effect of Co-doped Mn–Ni–In melt-spun ribbons

"Ribbon-shaped magnetocaloric materials are favorable to achieve high heat-transfer efficiencies due to their large specific surface area. In this work, Mn50Ni41−xIn9Cox (0 ≤ x ≤ 4) ribbons were prepared using a melt-spinning technique, and the corresponding phase transformation and magnetocalo...

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Detalhes bibliográficos
Autores: Yiqiao Yang, Zongbin Li, CESAR FIDEL SANCHEZ VALDES, JOSE LUIS SANCHEZ LLAMAZARES, Bo Yang, Yudong Zhang, Claude Esling, Xiang Zhao, Liang Zuo
Formato: artículo
Estado:Versión publicada
Fecha de publicación:2020
País:México
Recursos:Instituto Potosino de Investigación Científica y Tecnológica
Repositorio:Repositorio Institucional del IPICYT
OAI Identifier:oai:ipicyt.repositorioinstitucional.mx:1010/2341
Acesso em linha:http://ipicyt.repositorioinstitucional.mx/jspui/handle/1010/2341
Access Level:acceso embargado
Palavra-chave:info:eu-repo/classification/Autor/Induced shape recovery
info:eu-repo/classification/Autor/Room-temperature
info:eu-repo/classification/Autor/Martensitic transformations
info:eu-repo/classification/Autor/Giant
info:eu-repo/classification/cti/1
info:eu-repo/classification/cti/22
Descrição
Resumo:"Ribbon-shaped magnetocaloric materials are favorable to achieve high heat-transfer efficiencies due to their large specific surface area. In this work, Mn50Ni41−xIn9Cox (0 ≤ x ≤ 4) ribbons were prepared using a melt-spinning technique, and the corresponding phase transformation and magnetocaloric properties were studied. The large temperature gradient during melt-spinning caused the initial austenite in the ribbons to form typical columnar-shaped grains with a strong ⟨001⟩A preferred orientation perpendicular to the ribbon plane. After cooling, the ribbons undergo martensitic transformation from cubic austenite to monoclinic eight-layered modulated (8 M) martensite. High angle annular dark field-scanning transmission electron microscopy observations indicate that martensite lattice modulation is inhomogeneous at atomic scales. Co substitution for Ni not only strongly influences the phase transformation temperatures but also greatly enhances ferromagnetic coupling. As a result, an enlarged magnetization difference across the martensitic transformation under a field change of 5 T in the Mn50Ni38In9Co3 ribbon induces a large magnetic entropy change up to 12.1 J kg−1 K–1 and a refrigeration capacity of 197 J kg–1 around room temperature. In addition, a wide operational temperature region up to 31 K is obtained in the Mn50Ni37In9Co4 ribbon due to the enhanced sensitivity of the transformation temperature shift under a magnetic field."