DOI QR코드

DOI QR Code

Soft Magnetic Properties of Ring-Shaped Fe-Co-B-Si-Nb Bulk Metallic Glasses

  • Ishikawa, Takayuki (Department of Machine Intelligence and Systems Engineering, Faculty of Systems Science and Technology, Akita Prefectural University) ;
  • Tsubota, Takahiro (Department of Machine Intelligence and Systems Engineering, Faculty of Systems Science and Technology, Akita Prefectural University) ;
  • Bitoh, Teruo (Department of Machine Intelligence and Systems Engineering, Faculty of Systems Science and Technology, Akita Prefectural University)
  • 투고 : 2011.08.11
  • 심사 : 2011.09.15
  • 발행 : 2011.12.31

초록

The reduction of the Nb content in the $(Fe_{0.75}B_{0.20}Si_{0.05})_{96}Nb_4$ bulk metallic glass (BMG) has been studied. The glass-forming ability (GFA) is reduced by decreasing the Nb content, but it can be enhanced by replacing partially Fe by Co. Furthermore, the saturation magnetization of the $(Fe_{0.8}Co_{0.2})_{76}B_{18}Si_3Nb_3$ BMG is 1.35 T, being with 13% larger than that of the base alloy $(Fe_{0.75}B_{0.20}Si_{0.05})_{96}Nb_4$. $(Fe_{0.8}Co_{0.2})_{76}B_{18}Si_3Nb_3$ BMG exhibits slightly larger $B_{800}$ (the magnetic flux density at 800 A/m) and smaller core losses (20%-30%) compared with the commercial Fe-6.5 mass% Si steel.

키워드

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피인용 문헌

  1. Glass-Forming Ability and Magnetic Properties of $({\rm Fe}_{0.80}{\rm Co}_{0.20})_{96\hbox{-}{x}}{\rm B}_{{x}}{\rm Si}_{{1}}{\rm Nb}_{{3\hbox{-}{y}}}{\rm Y}_{{{\rm y}}}~({{x}}={15}, 17)$ Amorphous Alloys vol.50, pp.4, 2014, https://doi.org/10.1109/TMAG.2013.2287883
  2. Effects of temperature and gas phase impurities on the composition of Co-B alloy surface layers vol.89, pp.5, 2015, https://doi.org/10.1134/S0036024415050143
  3. Effect of Yttrium Addition on Glass-Forming Ability and Magnetic Properties of Fe–Co–B–Si–Nb Bulk Metallic Glass vol.5, pp.3, 2015, https://doi.org/10.3390/met5031127
  4. Glass-Forming Ability and Magnetization of (Fe, Co)-B-Si-(Nb, RE) (RE = Nd, Sm, Dy) Amorphous Alloys vol.65, pp.7, 2018, https://doi.org/10.2497/jjspm.65.395