咨询与建议

看过本文的还看了

相关文献

该作者的其他文献

文献详情 >Micromagnetism simulation on e... 收藏

Micromagnetism simulation on effects of soft phase size on Nd2Fe14B/α-Fe nanocomposite magnet with soft phase imbedded in hard phase

Micromagnetism simulation on effects of soft phase size on Nd_2Fe_(14)B/α-Fe nanocomposite magnet with soft phase imbedded in hard phase

作     者:Yu-Qing Li Ming Yue Yi Pen Hong-Guo Zhang 李玉卿;岳明;彭懿;张红国

作者机构:College of Materials Science and EngineeringBeijing University of TechnologyBeijing 100124China 

出 版 物:《Chinese Physics B》 (中国物理B(英文版))

年 卷 期:2018年第27卷第8期

页      面:529-534页

核心收录:

学科分类:07[理学] 0805[工学-材料科学与工程(可授工学、理学学位)] 0704[理学-天文学] 0702[理学-物理学] 

基  金:Project supported by the Key Program of the National Natural Science Foundation of China(Grant No.51331003) the International S&T Cooperation Program of China(Grant No.2015DFG52020) the General Program of Science and Technology Development Project of Beijing Municipal Education Commission,China(Grant No.KM201710005006) the State Key Laboratory of Advanced Metals and Materials,China(Grant No.2015-ZD02) 

主  题:micromagnetism simulation magnetization dynamics, Nd2Fe14B/a-Fe nanocomposite magnets 

摘      要:In this study, micromagnetism simulation by using timte dltterence method is cameo out on the Ncl21-el415/a-Fe nanocomposite magnet with soft phase imbedded in hard phase. The effects of soft magnetic phase size (S) on the magnetic properties and magnetic reversal modes are systematically analyzed. As S increases from 1 nm to 48 nm, the remanence (Jr) increases, while the coercivity (Hci) decreases, leading to the result that the magnetic energy prod- uct [(BH)max] first increases slowly, and then decreases rapidly, peaking at S = 24 nm with the (BH)max of 72.9 MGOe (1 MGOe = 7.95775 kJ.m-3). Besides, with the increase of S, the coercivity mechanism of the nanocomposite magnet changes from nucleation to pinning. Furthermore, by observing the magnetic moment evolution in demagnetization pro- cess, the magnetic reversal of the soft phase in the nanocomposite magnet can be divided into three modes with the increase of S: coherent rotation (S 〈 3 nm), quasi-coherent rotation (3 nm≤S 〈 36 nm), and the vortex-like rotation (S ≥36 nm).

读者评论 与其他读者分享你的观点

用户名:未登录
我的评分