Abstract:We consider in this paper the numerical approximation of a quasi-static contact problem in linear thermoelasticity that models the evolution of the temperature and displacement of an elastic, homogeneous, and isotropic body that may come in contact with an elastic obstacle. We propose a finite element method to numerically approximate the continuous solution. Convergence without any regularity assumptions is proved and error estimates are obtained if the continuous solution is sufficiently regular.
“…However, it is very difficult for us to obtain the analytical solutions of the generalized models with arbitrary initial-boundary conditions. Fortunately, a lot of numerical methods, such as, numerical integration methods [25][26][27], finite element methods [28][29][30][31], boundary element method [32], collocation methods [33][34][35][36] and finite difference methods [37][38][39][40][41], have been developed by scientists and engineers for them. However, mathematical analyses including convergence, stability, posteriori estimation, and energy conservation or dissipation, have not been studied for most of them.…”
Section: Mathematical Model and Related Studiesmentioning
This study is concerned with numerical solutions of a Magneto-Thermo-Elasticity (MTE) model via a combination of energy-conserving finite difference method (FDM) with Richardson extrapolation methods (REMs). Firstly, by introducing two auxiliary functions and using second-order centered FDM and Crank-Nicolson method to approximate spatial and temporal derivatives, respectively, a two-level energy-conserving FDM is established for a MTE model. The priori estimation, solvability, and convergence are derived rigorously by using the discrete energy method. Secondly, to improve computational efficiency, a class of REMs are also designed by constructing the symbolic expansion of numerical solutions. Finally, numerical results confirm the efficiency of the proposed algorithms and the exactness of the theoretical findings.
“…However, it is very difficult for us to obtain the analytical solutions of the generalized models with arbitrary initial-boundary conditions. Fortunately, a lot of numerical methods, such as, numerical integration methods [25][26][27], finite element methods [28][29][30][31], boundary element method [32], collocation methods [33][34][35][36] and finite difference methods [37][38][39][40][41], have been developed by scientists and engineers for them. However, mathematical analyses including convergence, stability, posteriori estimation, and energy conservation or dissipation, have not been studied for most of them.…”
Section: Mathematical Model and Related Studiesmentioning
This study is concerned with numerical solutions of a Magneto-Thermo-Elasticity (MTE) model via a combination of energy-conserving finite difference method (FDM) with Richardson extrapolation methods (REMs). Firstly, by introducing two auxiliary functions and using second-order centered FDM and Crank-Nicolson method to approximate spatial and temporal derivatives, respectively, a two-level energy-conserving FDM is established for a MTE model. The priori estimation, solvability, and convergence are derived rigorously by using the discrete energy method. Secondly, to improve computational efficiency, a class of REMs are also designed by constructing the symbolic expansion of numerical solutions. Finally, numerical results confirm the efficiency of the proposed algorithms and the exactness of the theoretical findings.
“…It can be assured due to [12] by assuming of thermally isolated lower and upper faces of the plate. The quasistatic case of such an approach has been solved numerically in [9]. We shall use the model derived in [13] under the assumption of a small change of temperature compared with its reference temperature.…”
We deal with a dynamic contact problem for a thermoelastic plate vibrating against a rigid obstacle. Dynamics is described by a hyperbolic variational inequality for deflections. The plate is subjected to a perpendicular force and to a heat source. The parabolic equation for the thermal strain resultant contains the time derivative of the deflection. We formulate a weak solution of the system and verify its existence using the penalization method.
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