RUS  ENG
Full version
JOURNALS // Zhurnal Vychislitel'noi Matematiki i Matematicheskoi Fiziki // Archive

Zh. Vychisl. Mat. Mat. Fiz., 2006 Volume 46, Number 3, Pages 407–420 (Mi zvmmf498)

This article is cited in 5 papers

Grid approximation of singularly perturbed parabolic equations in the presence of weak and strong transient layers induced by a discontinuous right-hand side

G. I. Shishkin

Institute of Mathematics and Mechanics, Ural Division, Russian Academy of Sciences, ul. S. Kovalevskoi 16, Yekaterinburg, 620219, Russia

Abstract: The initial value problem on a line for singularly perturbed parabolic equations with convective terms is investigated. The first-and the second-order space derivatives are multiplied by the parameters $\varepsilon_1$ and $\varepsilon_2$, respectively, which may take arbitrarily small values. The right-hand side of the equations has a discontinuity of the first kind on the set $\bar\gamma=[x=0]\times[0,T]$. Depending on the relation between the parameters, the appearing transient layers can be parabolic or regular, and the “intensity” of the layer (the maximum of the singular component) on the left and on the right of $\bar\gamma$ can be substantially different. If the parameter $\varepsilon_2$ at the convective term is finite, the transient layer is weak. For the initial value problems under consideration, the condensing grid method is used to construct finite difference schemes whose solutions converge (in the discrete maximum norm) to the exact solution uniformly with respect to $\varepsilon_1$ and $\varepsilon_2$ (when $\varepsilon_2$ is finite and, therefore, the transient layers are weak, no condensing grids are required).

Key words: singularly perturbed parabolic equations, transient layers of the solution, condensing grids, finite difference schemes.

UDC: 519.633

Received: 03.10.2005


 English version:
Computational Mathematics and Mathematical Physics, 2006, 46:3, 388–401

Bibliographic databases:


© Steklov Math. Inst. of RAS, 2026