A simple thermodynamic model for rigid ferromagnets with hysteresis phenomena is constructed on the basis of the second principle of thermodynamics and the time-evolution equation of the magnetization which is subjected to satisfying the former. Both Landau-Lifshitz and longitudinal relaxation effects are obtained for a nonlinear magnetic material in which the magnetization has not reached saturation and is subjected to the influence of temperature. The possibilities of extending the obtained results to the case of elastic ferromagnets and using the obtained equations in the description of fluid suspensions of magnetic particles are briefly explored. The approach in fact belongs in the thermodynamic theory of internal variables which therefore looks promising for the description of phase-transition phenomena.
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