Conservative numerical method for a system of semilinear singularly perturbed parabolic reaction‐diffusion equations

On a vertical strip, a Dirichlet problem is considered for a system of two semilinear singularly perturbed parabolic reaction‐diffusion equations connected only by terms that do not involve derivatives. The highest‐order derivatives in the equations, having divergent form, are multiplied by the per...

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Main Authors: Lidia Shishkina, Grigorii Shishkin
Format: Article
Language:English
Published: Vilnius Gediminas Technical University 2009-06-01
Series:Mathematical Modelling and Analysis
Subjects:
Online Access:https://journals.vgtu.lt/index.php/MMA/article/view/6541
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spelling doaj-45cc724cdb5749c8896ee5a149e111d72021-07-02T11:37:02ZengVilnius Gediminas Technical UniversityMathematical Modelling and Analysis1392-62921648-35102009-06-0114210.3846/1392-6292.2009.14.211-228Conservative numerical method for a system of semilinear singularly perturbed parabolic reaction‐diffusion equationsLidia Shishkina0Grigorii Shishkin1Institute of Mathematics and Mechanics, Russian Academy of Sciences; Ekaterinburg 620219, GSP-384, RussiaInstitute of Mathematics and Mechanics, Russian Academy of Sciences; Ekaterinburg 620219, GSP-384, Russia On a vertical strip, a Dirichlet problem is considered for a system of two semilinear singularly perturbed parabolic reaction‐diffusion equations connected only by terms that do not involve derivatives. The highest‐order derivatives in the equations, having divergent form, are multiplied by the perturbation parameter e ; ϵ ∈ (0,1]. When ϵ → 0, the parabolic boundary layer appears in a neighbourhood of the strip boundary. Using the integro‐interpolational method, conservative nonlinear and linearized finite difference schemes are constructed on piecewise‐uniform meshes in the x 1 ‐axis (orthogonal to the boundary) whose solutions converge ϵ‐uniformly at the rate O (N1−2 ln2 N 1 + N 2 −2 + N 0 −1). Here N 1 + 1 and N 0 + 1 denote the number of nodes on the x 1‐axis and t‐axis, respectively, and N 2 + 1 is the number of nodes in the x 2‐axis on per unit length. First published online: 14 Oct 2010 https://journals.vgtu.lt/index.php/MMA/article/view/6541boundary value problemvertical stripsystem of semilinear equationsparabolic reaction‐diffusion equationsperturbation parameter ϵparabolic boundary layer
collection DOAJ
language English
format Article
sources DOAJ
author Lidia Shishkina
Grigorii Shishkin
spellingShingle Lidia Shishkina
Grigorii Shishkin
Conservative numerical method for a system of semilinear singularly perturbed parabolic reaction‐diffusion equations
Mathematical Modelling and Analysis
boundary value problem
vertical strip
system of semilinear equations
parabolic reaction‐diffusion equations
perturbation parameter ϵ
parabolic boundary layer
author_facet Lidia Shishkina
Grigorii Shishkin
author_sort Lidia Shishkina
title Conservative numerical method for a system of semilinear singularly perturbed parabolic reaction‐diffusion equations
title_short Conservative numerical method for a system of semilinear singularly perturbed parabolic reaction‐diffusion equations
title_full Conservative numerical method for a system of semilinear singularly perturbed parabolic reaction‐diffusion equations
title_fullStr Conservative numerical method for a system of semilinear singularly perturbed parabolic reaction‐diffusion equations
title_full_unstemmed Conservative numerical method for a system of semilinear singularly perturbed parabolic reaction‐diffusion equations
title_sort conservative numerical method for a system of semilinear singularly perturbed parabolic reaction‐diffusion equations
publisher Vilnius Gediminas Technical University
series Mathematical Modelling and Analysis
issn 1392-6292
1648-3510
publishDate 2009-06-01
description On a vertical strip, a Dirichlet problem is considered for a system of two semilinear singularly perturbed parabolic reaction‐diffusion equations connected only by terms that do not involve derivatives. The highest‐order derivatives in the equations, having divergent form, are multiplied by the perturbation parameter e ; ϵ ∈ (0,1]. When ϵ → 0, the parabolic boundary layer appears in a neighbourhood of the strip boundary. Using the integro‐interpolational method, conservative nonlinear and linearized finite difference schemes are constructed on piecewise‐uniform meshes in the x 1 ‐axis (orthogonal to the boundary) whose solutions converge ϵ‐uniformly at the rate O (N1−2 ln2 N 1 + N 2 −2 + N 0 −1). Here N 1 + 1 and N 0 + 1 denote the number of nodes on the x 1‐axis and t‐axis, respectively, and N 2 + 1 is the number of nodes in the x 2‐axis on per unit length. First published online: 14 Oct 2010
topic boundary value problem
vertical strip
system of semilinear equations
parabolic reaction‐diffusion equations
perturbation parameter ϵ
parabolic boundary layer
url https://journals.vgtu.lt/index.php/MMA/article/view/6541
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