The Barkhausen noise was measured as the change of line width(39 ~ 1.22 ㎜) and scratching angle(90˚ - 50˚) with respect of rolling direction in grain-oriented 3% Si-Fe of 0.30 and 0.27 ㎜ thickness. The two peak phenomena of the noise envelope ob...
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https://www.riss.kr/link?id=A76075400
1994
Korean
428
KCI등재,ESCI
학술저널
142-149(8쪽)
0
상세조회0
다운로드다국어 초록 (Multilingual Abstract)
The Barkhausen noise was measured as the change of line width(39 ~ 1.22 ㎜) and scratching angle(90˚ - 50˚) with respect of rolling direction in grain-oriented 3% Si-Fe of 0.30 and 0.27 ㎜ thickness. The two peak phenomena of the noise envelope ob...
The Barkhausen noise was measured as the change of line width(39 ~ 1.22 ㎜) and scratching angle(90˚ - 50˚) with respect of rolling direction in grain-oriented 3% Si-Fe of 0.30 and 0.27 ㎜ thickness. The two peak phenomena of the noise envelope observed for non-scratching and scratching of line width 39 ㎜ was explained by large activation energy during 180˚ domain wall nucleation and annihilation processes. The amplitudes of the noise envelpoes were decreased as the decrement of scratching line width, but did not almost changed below line width of 9.75 ㎜. It was explained that the decrease in the envelope with increasing scratching number is associated with lower activation energy of 180˚ domain nucleation and annihilation in the vicinity of the scratching area. The noise power was decreased as narrower line width. The dependence of the power on the scratching angle was sharpest decreaded at the 50 angle.
기공율, 응력 및 입자 크기가 B-H Hysteresis loop 특성에 미치는 영향 연구
주파수 변화에 따른 다결정 MgFe₂O₄의 초기 투자율 특성 연구