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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

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