
doi: 10.1137/0719082
In this paper the implicit time discretization of $E_t - \nabla \cdot K\nabla T = f$, the enthalpy formulation of the Stef an problem, is considered. This generates the algebraic system $E + A\beta (E) = \eta $, where E, $\beta (E)$, $\eta \in {}^ + \mathbb{R}^L $, A is an M-matrix and $\beta (E)$ is the “inverse” of the enthalpy function. The algebraic equation is solved by a modification of the Gauss–Seidel method and convergence is proved. The existence and uniqueness of a weak solution with $T \in W_2^{1,0} (Q_T )$ is established by Rothe’s method. An application to thermal energy storage units which utilize phase change materials is given. Heat transfer via both diffusion and convection of the liquid phase change material is considered.
Finite difference methods for boundary value problems involving PDEs, convergence, Thermodynamics of continua, Method of lines for boundary value problems involving PDEs, Rothe's method, Heat equation, diffusion, weak solution, Gauss-Seidel method, Numerical solution of discretized equations for boundary value problems involving PDEs, Stefan problem, implicit time discretization, Applications to the sciences, heat transfer, liquid phase change, Free boundary problems for PDEs, M-matrix, convection, enthalpy formulation
Finite difference methods for boundary value problems involving PDEs, convergence, Thermodynamics of continua, Method of lines for boundary value problems involving PDEs, Rothe's method, Heat equation, diffusion, weak solution, Gauss-Seidel method, Numerical solution of discretized equations for boundary value problems involving PDEs, Stefan problem, implicit time discretization, Applications to the sciences, heat transfer, liquid phase change, Free boundary problems for PDEs, M-matrix, convection, enthalpy formulation
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