Coercivity mechanism of sintered NdFeB magnets having high coercivities

1990 ◽  
Vol 67 (9) ◽  
pp. 4750-4752 ◽  
Author(s):  
A. Fukuno ◽  
K. Hirose ◽  
T. Yoneyama
2014 ◽  
Vol 802 ◽  
pp. 558-562 ◽  
Author(s):  
Marcos Flavio de Campos ◽  
Fernanda A.S. da Silva ◽  
José Adilson de Castro

The volume fraction of the single domain size particles can be directly estimated from the initial magnetization of thermally demagnetized magnets. Multi-domain grains present initial magnetization curve with high initial susceptibility, whereas single-domain grains present low susceptibility initial magnetization curve. In the case of single domain size particles, the coercivity mechanism is coherent rotation and the Stoner-Wohlfarth (SW) model can be applied. From the initial magnetization curve of magnets, the volume fraction of grains with diameter less than 0.3 micrometers can be estimated in NdFeB magnets. This is possible because the Nd2Fe14B phase is single domain below 0.3 micrometers.


2011 ◽  
Vol 179-180 ◽  
pp. 751-756
Author(s):  
Peng Yue Zhang ◽  
Hong Liang Ge ◽  
Min Xiang Pan ◽  
Qiong Wu ◽  
Hang Fu Yang ◽  
...  

The effects of Zr addition on the microstructure and magnetic properties of the sintered NdFeB magnets were investigated by X-ray diffraction (XRD) and BH magnetic tester. The XRD analysis showed that both the Zr-free and Zr-doped samples are composed of main amount of Tetragonal phase Nd2Fe14B (P42/mnm) and trace amount of Nd-rich phase, but adding Zr reduces significantly the values of pole density factor of (004), (006) and (008) crystal faces for the sintered Nd(Fe,Zr)B magnets estimated by Horta-formula. Accordingly, the coercivity of the sample with Zr addition is reduced from 2038 kA/m down to 1951 kA/m. The study of the Kronmüller-plot shows that the nucleation is the dominating mechanism for the magnetization reversal in these two kinds of magnets, and two microstructural parameters of αk and Neff are obtained also.


2014 ◽  
Vol 775-776 ◽  
pp. 437-442 ◽  
Author(s):  
Marcos Flavio de Campos

In the first part of this article, the SW-CLC (Stoner-Wohlfarth with CLC modification) model is discussed for nanocrystalline magnets, as melt-spun exchange coupled NdFeB. In the second part, the effect of grain size of coercivity for large grain size, above the single domain particle size, is addressed. The Kondorsky law observed for large grain size only can be due to domain wall displacement phenomena, where there is nucleus expansion. There are two main situations, one for nanocrystalline grain size, where the SW-CLC model is obeyed, and other for large grain size, where the coercive field decreases proportionally to the square root of the grain size.


1988 ◽  
Vol 49 (C8) ◽  
pp. C8-655-C8-656 ◽  
Author(s):  
A. Handstein ◽  
J. Schneider ◽  
U. Heinecke ◽  
R. Grössinger ◽  
H. Sassik

2021 ◽  
Vol 860 ◽  
pp. 158424
Author(s):  
Younghwan Jeon ◽  
Jungho Hur ◽  
Gwan Yoon Jeong ◽  
Sungjune Sohn ◽  
Jaeyeong Park

2006 ◽  
Vol 05 (04n05) ◽  
pp. 627-631 ◽  
Author(s):  
M. J. SUN ◽  
G. P. ZHAO ◽  
J. LIANG ◽  
G. ZHOU ◽  
H. S. LIM ◽  
...  

A simplified micromagnetic model has been proposed to calculate the hysteresis loops of nanostructured permanent magnets for various configurations, including thin films, exchange-coupled double-layer systems and bulk materials. The reversal part of the hysteresis is based on the Stoner–Wohlfarth coherent rotational model and the coercivity mechanism is due mainly to the motion of the transition region (a domain wall like magnetic moment distribution in the grain boundary). The elements of nucleation and pinning models are also incorporated.


1996 ◽  
Vol 32 (5) ◽  
pp. 4407-4409 ◽  
Author(s):  
N.C. Ku ◽  
C.-D. Qin ◽  
C.C. Yu ◽  
D.H.L. Ng

2015 ◽  
Vol 51 (11) ◽  
pp. 1-4
Author(s):  
Z. W. Liu ◽  
L. Z. Zhao ◽  
S. L. Hu ◽  
H. Y. Yu ◽  
X. C. Zhong ◽  
...  

2012 ◽  
Vol 19 (3) ◽  
pp. 236-239 ◽  
Author(s):  
Ai-zhi Sun ◽  
Shen Wu ◽  
Wen-huan Xu ◽  
Jin Wang ◽  
Qian Zhang ◽  
...  
Keyword(s):  

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