4.2 Hard magnetic materials
4.2 Hard magnetic materials
4.2 Hard magnetic materials
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Crystalline structure of R 2 Fe 14 B<br />
NdFeB magnets<br />
I-T curves for R 2 Fe 14 B<br />
s I<br />
Nucleation type magnets<br />
Magnetization reversal in sintered 2-14-1 magnets<br />
occurs by nucleation and growth of reversal domains.<br />
According to Kronmuller the coercivity is given by<br />
2Ku<br />
IHC = aKa eff<br />
Ψ<br />
−N I<br />
Is<br />
Here, a K describes the micro<strong>magnetic</strong> effects of anisotropy, wall width, and inhomogeneity size;<br />
a ψ describes the effects of grain misallignment. These two factors differ depending on whether wall<br />
motion is limited by pinning or nucleation. Experiments support nuclation form of this model.