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Curie-Weiss Theory Classical Approach

We suspect that spontaneous magnetism must have something to do with the d-electrons in the transition metals and the/-electrons in the rare earth metals since they have unpaired spins. We can postulate that there must be some self-generated ordering force that keeps [Pg.500]

Putting this result into Equation 25.29, we can solve for the magnetization as a function of temperature  [Pg.501]

Solutions exist for T Tq only if the applied field H 0. Equation 25.29 may be approximated by [Pg.501]

Universal magnetization versus reduced temperature curve. The model gives very good agreement with measured data. [Pg.502]

It should also be mentioned that peff obtained from the saturation magnetism was only 2.22, whereas the value for Fe with four impaired spins estimated from 2y/S (S + 1) = 4.90. There are several possible reasons for this lower value of peff in the pure metal spin-orbit interactions, interference with the conduction electrons, and the Fermi level cutting off some of these higher energy states. Also some fraction of the d-electrons participate in forming covalent bonds. It is not a perfect theory. [Pg.502]


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