“…The model provides a detailed depiction of the three-dimensional evolution of thermodynamic and electromagnetic properties inherent in ferromagnetic materials, which can account for temperature-induced transitions from the paramagnetic to the ferromagnetic regime. The model is applicable to a wide range of temperatures [9], while the well-known Landau-Lifschitz equation can only describe magnetization dynamics at low temperatures [10][11][12][13]. The evolution of the ferromagnetic material is described by the phase transition equations referenced in [6], which are formulated as follows:…”
Section: Introductionmentioning
confidence: 99%
“…If we regard polarization P as an internal field, then we can derive the electric polarization Equation ( 7), more details can be found in [20]. Substituting (11) into (10), we obtain a couple system of M, θ, E, H, and P, that is, (3)- (7).…”
This paper deals with a phase transition model with polarization which describes the thermodynamic, electromagnetic, and polarization properties of ferromagnetic–ferroelectric materials. The existence of the global weak solution for the phase transition equations with polarization is rigorously established through the viscosity vanishing argument.
“…The model provides a detailed depiction of the three-dimensional evolution of thermodynamic and electromagnetic properties inherent in ferromagnetic materials, which can account for temperature-induced transitions from the paramagnetic to the ferromagnetic regime. The model is applicable to a wide range of temperatures [9], while the well-known Landau-Lifschitz equation can only describe magnetization dynamics at low temperatures [10][11][12][13]. The evolution of the ferromagnetic material is described by the phase transition equations referenced in [6], which are formulated as follows:…”
Section: Introductionmentioning
confidence: 99%
“…If we regard polarization P as an internal field, then we can derive the electric polarization Equation ( 7), more details can be found in [20]. Substituting (11) into (10), we obtain a couple system of M, θ, E, H, and P, that is, (3)- (7).…”
This paper deals with a phase transition model with polarization which describes the thermodynamic, electromagnetic, and polarization properties of ferromagnetic–ferroelectric materials. The existence of the global weak solution for the phase transition equations with polarization is rigorously established through the viscosity vanishing argument.
In this paper we study numerical methods for solving a system of quasilinear stochastic partial differential equations known as the stochastic Landau–Lifshitz–Bloch (LLB) equation on a bounded domain in ${\mathbb{R}}^{d}$ for $d=1,2$. Our main results are estimates of the rate of convergence of the Finite Element Method to the solutions of stochastic LLB. To overcome the lack of regularity of the solution in the case $d=2$, we propose a Finite Element scheme for a regularized version of the equation. We then obtain error estimates of numerical solutions and for the solution of the regularized equation as well as the rate of convergence of this solution to the solution of the stochastic LLB equation. As a consequence, the convergence in probability of the approximate solutions to the solution of the stochastic LLB equation is derived. A stronger result is obtained in the case $d=1$ due to a new regularity result for the LLB equation which allows us to avoid regularization.
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