Recently, Fe-rich alloys with ThMn12 structure have attracted much attention as next generation permanent magnet materials. Among them, Sm(Fe<SUB>0.8</SUB>Co<SUB>0.2</SUB>)<SUB>11</SUB>Ti alloy shows good magnetic p...
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https://www.riss.kr/link?id=A106925239
2020
Korean
428
KCI등재,ESCI
학술저널
80-84(5쪽)
0
상세조회0
다운로드다국어 초록 (Multilingual Abstract)
Recently, Fe-rich alloys with ThMn12 structure have attracted much attention as next generation permanent magnet materials. Among them, Sm(Fe<SUB>0.8</SUB>Co<SUB>0.2</SUB>)<SUB>11</SUB>Ti alloy shows good magnetic p...
Recently, Fe-rich alloys with ThMn12 structure have attracted much attention as next generation permanent magnet materials. Among them, Sm(Fe<SUB>0.8</SUB>Co<SUB>0.2</SUB>)<SUB>11</SUB>Ti alloy shows good magnetic properties, however the low coercivity problem is still to be solved. In order to improve the coercivity, Sm(Fe<SUB>0.8</SUB>Co<SUB>0.2</SUB>)<SUB>11</SUB>Ti bulk samples were prepared by adding non-magnetic Sm<SUB>7</SUB>Cu₃ powders (0, 5, and 10 wt%). The crystallographic and magnetic properties of Sm(Fe<SUB>0.8</SUB>Co<SUB>0.2</SUB>)<SUB>11</SUB>Ti added Sm7Cu₃ have been investigated by using X-ray
diffractometer (XRD), scaning electron microscope (SEM), and vibrating sample magnetometer (VSM). The phase identity and volume fraction of Sm(Fe<SUB>0.8</SUB>Co<SUB>0.2</SUB>)<SUB>11</SUB>Ti powders were determined by using Rietveld refinement. The phase distribution of grains and grain boundaries was analyzed by using SEM. With increasing Sm<SUB>7</SUB>Cu₃ content, the value of saturation magnetization of Sm(Fe<SUB>0.8</SUB>Co<SUB>0.2</SUB>)<SUB>11</SUB>Ti bulk samples decreased, while their coercivity increased by about 67% with an addition of a non-magnetic phase.
초고속 스트레인 펄스에 의한 자성체 동역학: 응용과 전망