欢迎登录材料期刊网

材料期刊网

高级检索

Dynamic crystallization was introduced to improve the magnetic properties of NdFeB nanocrystalline permanent magnets by optimizing microstructure. The microstructure was studied by X-ray diffraction (XRD) and transmission electron microscopy (TEM). It has been determined that, compared with the conventional heat treatment, dynamic crystallization can shorten the crystallization time. Moreover, dynamic crystallization can refine grains, enhance the exchange-coupled interaction among grains, and promote the magnetic properties. As a result, the optimal magnetic properties of Nd10.5(FeCoZr)83.4B6.1(Br=0.685T, Hci =732 kA·m -1 , Hcb =429 kA·m-1 ,( BH )m=75 kJ·m -3 ) are obtained after dynamic crystallization heat treatment at 700 ℃ for 10 min.

参考文献

[1] Sagawa M;Fujimura S;Togawa N et al.New material for permanent magnets on a base of Nd and Fe[J].Journal of Applied Physics,1984,55:2083.
[2] Dong Shengzhi;Li Xiumei;Li Wei et al.Structure and magnetic properties of nanocomposite alloy Nd4.5Fe76.3Ga0.2Co1.0B18[J].Acta Physica Sinica,1999,48(zk):S63.
[3] Fischer R;Schrefl T;Kronmuller H et al.Grain-size dependence of remanence and coercive field of isotropic nanocrystalline composite permanent magnets[J].Journal of Magnetism and Magnetic Materials,1996,153:35.
[4] 刘颖,陈悦,涂铭旌,王永强,赵文金,彭倩.热处理对非晶态合金Nd9(FeCoZrAl)85B6磁性能的影响[J].中国稀土学报,2000(02):112-115.
[5] 查五生,刘颖,高升吉,涂铭旌.高矫顽力低稀土含量快淬Pr10.5(FeCoZr)83.5B6粘结磁体制备[J].稀有金属材料与工程,2004(01):75-78.
[6] 王占勇,周邦新,徐晖,倪建森.快淬双相纳米复合稀土永磁材料的晶化研究[J].稀有金属材料与工程,2005(01):1-6.
[7] Gao Youhui;Weng Yuqing;Park Eon Byung;Yang Choong Jin;Zhu Jinghan .Enhanced exchange coupled interaction in nanocrystalline Nd2Fe14B/Fe3B+αFe alloys with improved microstructure[J].Journal of Magnetism and Magnetic Materials,1999(1/2):146-152.
[8] Chiriac H;Marinescu M;Buschow K H J et al.Influence of the annealing procedures on magnetic properties of α-Fe/Nd2Fe14B nanocrystalline alloys[J].Journal of Magnetism and Magnetic Materials,1999,202:22.
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%