x M x C y (M=Ti, Zr, Hf, V and Ge; x = 0-.3 and y = 0-.1) ribbons was studied. Based on the XRD and the TEM analyses, a pure 1:7 phase could be formed for the C-containing ribbons with M= Ti and Ge. However, carbide phases, i.e., Sm2C3 for M=Zr and Hf, and SmCoC2 for M=V, respectively, were found. Nevertheless, a slight C addition may effectively refine the microstructure and improve both the intrinsic coercvity and the magnetic energy product in all the studied ribbons. Among them, the SmCo6.9V0.1C0.1 ribbons with σ r = 58.7 emu/g, i H c = 13.5 kOe and (BH) max = 9.3 MGOe, and the SmCo6.9Hf0.1C0.1 ribbons with σ r = 61.6 emu/g, i H c = 11.8 kOe and (BH) max = 10.3 MGOe are most suitable for the bonded magnet applications." />
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Effect of a carbon additive on the TbCu7-type melt-spun Sm(Co, M)7 (M=Ti, Zr, Hf, V and Ge) ribbons
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  • 作者:Chih-Chieh Hsieh (1)
    Shih-Teng Huang (1)
    Jin-Sheng Guo (1)
    Chih-Wei Shih (1)
    Wen-Cheng Chang (1)
    Huang-Wei Chang (2)
    Chun-Chung Shaw (3)
  • 关键词:Cystal structure ; Melt spinning ; Permanent magnet ; TbCu7
  • 刊名:Journal of the Korean Physical Society
  • 出版年:2013
  • 出版时间:August 2013
  • 年:2013
  • 卷:63
  • 期:3
  • 页码:401-404
  • 全文大小:214KB
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  • 作者单位:Chih-Chieh Hsieh (1)
    Shih-Teng Huang (1)
    Jin-Sheng Guo (1)
    Chih-Wei Shih (1)
    Wen-Cheng Chang (1)
    Huang-Wei Chang (2)
    Chun-Chung Shaw (3)

    1. Department of Physics, National Chung Cheng University, Chia-yi, 62102, Taiwan, R.O.C.
    2. Department of Chemistry, Tunghai University, Taichung, 40704, Taiwan, R.O.C.
    3. Super Electronics Co. Ltd, Taipei, 11141, Taiwan, R.O.C.
  • ISSN:1976-8524
文摘
The effect of a carbon additive on the microstructure and the magnetic properties of melt-spun SmCo7?em class="a-plus-plus">x M x C y (M=Ti, Zr, Hf, V and Ge; x = 0-.3 and y = 0-.1) ribbons was studied. Based on the XRD and the TEM analyses, a pure 1:7 phase could be formed for the C-containing ribbons with M= Ti and Ge. However, carbide phases, i.e., Sm2C3 for M=Zr and Hf, and SmCoC2 for M=V, respectively, were found. Nevertheless, a slight C addition may effectively refine the microstructure and improve both the intrinsic coercvity and the magnetic energy product in all the studied ribbons. Among them, the SmCo6.9V0.1C0.1 ribbons with σ r = 58.7 emu/g, i H c = 13.5 kOe and (BH) max = 9.3 MGOe, and the SmCo6.9Hf0.1C0.1 ribbons with σ r = 61.6 emu/g, i H c = 11.8 kOe and (BH) max = 10.3 MGOe are most suitable for the bonded magnet applications.

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