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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Vilnius Gediminas Technical University
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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
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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 |
work_keys_str_mv |
AT lidiashishkina conservativenumericalmethodforasystemofsemilinearsingularlyperturbedparabolicreactiondiffusionequations AT grigoriishishkin conservativenumericalmethodforasystemofsemilinearsingularlyperturbedparabolicreactiondiffusionequations |
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1721330860920143872 |