A Finite Difference Method for Two-Phase Parabolic Obstacle-like Problem

In this paper we treat the numerical approximation of the two-phase parabolic obstacle-like problem: \[\Delta u -u_t=\lambda^+\cdot\chi_{\{u>0\}}-\lambda^-\cdot\chi_{\{u<0\}},\quad (t,x)\in (0,T)\times\Omega,\] where $T < \infty, \lambda^+ ,\lambda^- > 0$ are Lipschitz continuous functi...

Full description

Bibliographic Details
Main Author: Avetik Arakelyan
Format: Article
Language:English
Published: Republic of Armenia National Academy of Sciences 2015-05-01
Series:Armenian Journal of Mathematics
Online Access:http://www.armjmath.sci.am/index.php/ajm/article/view/109
id doaj-fe84ec550b2244e3a0928a8ff15a2466
record_format Article
spelling doaj-fe84ec550b2244e3a0928a8ff15a24662020-11-25T01:38:19ZengRepublic of Armenia National Academy of SciencesArmenian Journal of Mathematics1829-11632015-05-0171A Finite Difference Method for Two-Phase Parabolic Obstacle-like ProblemAvetik Arakelyan0Institute of mathematics, National Academy of Sciences of Armenia Bagramian ave. 24B, 0019 Yerevan, Armenia In this paper we treat the numerical approximation of the two-phase parabolic obstacle-like problem: \[\Delta u -u_t=\lambda^+\cdot\chi_{\{u>0\}}-\lambda^-\cdot\chi_{\{u<0\}},\quad (t,x)\in (0,T)\times\Omega,\] where $T < \infty, \lambda^+ ,\lambda^- > 0$ are Lipschitz continuous functions, and $\Omega\subset\mathbb{R}^n$ is a bounded domain. We introduce a certain variation form, which allows us to define a notion of viscosity solution. We use defined viscosity solutions framework to apply Barles-Souganidis theory. The numerical projected Gauss-Seidel method is constructed. Although the paper is devoted to the parabolic version of the two-phase obstacle-like problem, we prove convergence of the discretized scheme to the unique viscosity solution for both two-phase parabolic obstacle-like and standard two-phase membrane problem. Numerical simulations are also presented. http://www.armjmath.sci.am/index.php/ajm/article/view/109
collection DOAJ
language English
format Article
sources DOAJ
author Avetik Arakelyan
spellingShingle Avetik Arakelyan
A Finite Difference Method for Two-Phase Parabolic Obstacle-like Problem
Armenian Journal of Mathematics
author_facet Avetik Arakelyan
author_sort Avetik Arakelyan
title A Finite Difference Method for Two-Phase Parabolic Obstacle-like Problem
title_short A Finite Difference Method for Two-Phase Parabolic Obstacle-like Problem
title_full A Finite Difference Method for Two-Phase Parabolic Obstacle-like Problem
title_fullStr A Finite Difference Method for Two-Phase Parabolic Obstacle-like Problem
title_full_unstemmed A Finite Difference Method for Two-Phase Parabolic Obstacle-like Problem
title_sort finite difference method for two-phase parabolic obstacle-like problem
publisher Republic of Armenia National Academy of Sciences
series Armenian Journal of Mathematics
issn 1829-1163
publishDate 2015-05-01
description In this paper we treat the numerical approximation of the two-phase parabolic obstacle-like problem: \[\Delta u -u_t=\lambda^+\cdot\chi_{\{u>0\}}-\lambda^-\cdot\chi_{\{u<0\}},\quad (t,x)\in (0,T)\times\Omega,\] where $T < \infty, \lambda^+ ,\lambda^- > 0$ are Lipschitz continuous functions, and $\Omega\subset\mathbb{R}^n$ is a bounded domain. We introduce a certain variation form, which allows us to define a notion of viscosity solution. We use defined viscosity solutions framework to apply Barles-Souganidis theory. The numerical projected Gauss-Seidel method is constructed. Although the paper is devoted to the parabolic version of the two-phase obstacle-like problem, we prove convergence of the discretized scheme to the unique viscosity solution for both two-phase parabolic obstacle-like and standard two-phase membrane problem. Numerical simulations are also presented.
url http://www.armjmath.sci.am/index.php/ajm/article/view/109
work_keys_str_mv AT avetikarakelyan afinitedifferencemethodfortwophaseparabolicobstaclelikeproblem
AT avetikarakelyan finitedifferencemethodfortwophaseparabolicobstaclelikeproblem
_version_ 1725054560039337984