Optimal design of sintered Ce9Nd21FebalB1 magnets with a low-melting-point (Ce,Nd)-rich phase
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  • 作者:Shu-lin Huang (1) (2) (3)
    Hai-bo Feng (1) (3)
    Ming-gang Zhu (1) (3)
    An-hua Li (1) (3)
    Yan-feng Li (1) (3)
    Ya-chao Sun (1) (3)
    Yue Zhang (2)
    Wei Li (1) (3)

    1. Functional Materials Research Institute
    ; Central Iron and Steel Research Institute ; Beijing ; 100081 ; China
    2. School of Materials Science and Engineering
    ; University of Science and Technology Beijing ; Beijing ; 100083 ; China
    3. Beijing Key Laboratory of Precision Alloys
    ; Beijing ; 100081 ; China
  • 关键词:magnets ; liquid phases ; eutectic point ; enrichment ; optimal design
  • 刊名:International Journal of Minerals, Metallurgy, and Materials
  • 出版年:2015
  • 出版时间:April 2015
  • 年:2015
  • 卷:22
  • 期:4
  • 页码:417-422
  • 全文大小:2,465 KB
  • 参考文献:1. Yu, LQ, Zhang, J, Hu, SQ, Han, ZD, Yan, M (2008) Production for high thermal stability NdFeB magnets. J. Magn. Magn. Mater. 320: pp. 1427 CrossRef
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  • 刊物类别:Chemistry and Materials Science
  • 刊物主题:Materials Science
    Metallic Materials
    Mineral Resources
  • 出版者:Journal Publishing Center of University of Science and Technology Beijing, in co-publication with Sp
  • ISSN:1869-103X
文摘
A systemic investigation was done on the chemistry and crystal structure of boundary phases in sintered Ce9Nd21FebalB1 (wt%) magnets. Ce2Fe14B is believed to be more soluble in the rare-earth (RE)-rich liquid phase during the sintering process. Thus, the grain size and oxygen content were controlled via low-temperature sintering, resulting in high coercivity and maximum energy products. In addition, Ce formed massive agglomerations at the triple-point junctions, as confirmed by elemental mapping results. Transmission electron microscopy (TEM) images indicated the presence of (Ce,Nd)O x phases at grain boundaries. By controlling the composition and optimizing the preparation process, we successfully obtained Ce9Nd21FebalB1 sintered magnets; the prepared magnets exhibited a residual induction, coercivity, and energy product of 1.353 T, 759 kA/m, and 342 kJ/m3, respectively.

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