4.2 Hard magnetic materials
4.2 Hard magnetic materials
4.2 Hard magnetic materials
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The coercivity of the hexagonal ferrites is limitted by nucleation; once a domain wall exists in a<br />
particle, it moves with ease through the particle under an applied field. However, wall motion<br />
does not appear to propagate from grain to grain. Thus, the coercivity of hexagonal ferrites can<br />
be described by the mechanism of single-domain particle magnetization with the magnetocrystalline<br />
anisotropy.<br />
Commercial ferrite magnets<br />
I (mT)<br />
400<br />
200<br />
0<br />
SW: Stoner-Wohlfarth model<br />
K 1 = 3.4610 5 J/m 3<br />
1.2: Anisotropic magnets<br />
3: Isotropic magnet