Abstract
According to the classical theory of Weiβ, on a microscopic scale a ferromagnetic body is magnetically saturated (|M| =M 0: constant) and is composed by uniformly magnetized regions separated by thin transition layers.
At equilibrium this corresponds to the minimization of the magnetic energy functional
under the above constraint; this problem has at least one solutionM of classH 1, which in general is not unique. The evolution is governed by Landau-Lifshitz’ equations
; these are coupled with Maxwell’s equations. An existence result based on the energy estimate and some complementary properties are proved for the corresponding variational formulation. Finally the magnetostrictive effect is included.
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Visintin, A. On Landau-Lifshitz’ equations for ferromagnetism. Japan J. Appl. Math. 2, 69–84 (1985). https://doi.org/10.1007/BF03167039
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DOI: https://doi.org/10.1007/BF03167039