On Conditioning of a Schwarz Method for Singularly Perturbed Convection-diffusion Equations in the Case of Disturbances in the Data of the Boundary-value Problem
Gespeichert in:
Verfasser / Beitragende:
[Gregorii I. Shishkin]
Ort, Verlag, Jahr:
2003
Enthalten in:
Computational Methods in Applied Mathematics, 3/3(2003), 459-487
Format:
Artikel (online)
Online Zugang:
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| 024 | 7 | 0 | |a 10.2478/cmam-2003-0030 |2 doi |
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| 100 | 1 | |a Shishkin |D Gregorii I. |u Institute of Mathematics and Mechanics, Ural Branch of the Russian Academy of Sciences, 16 S. Kovalevskaya Str., 620219 Ekaterinburg, Russia. | |
| 245 | 1 | 0 | |a On Conditioning of a Schwarz Method for Singularly Perturbed Convection-diffusion Equations in the Case of Disturbances in the Data of the Boundary-value Problem |h [Elektronische Daten] |c [Gregorii I. Shishkin] |
| 520 | 3 | |a In this paper we discuss conditioning of a discrete Schwarz method on piecewise-uniform meshes with an example of a one-dimensional singularly perturbed boundary-value problem. We consider a Dirichlet problem for singularly perturbed ordinary differential equations with convection terms and a small perturbation parameter ε. To solve the problem numerically we use an ε-uniformly convergent (in the maximum norm) difference scheme on special piecewise-uniform meshes. For this base scheme we construct a decomposition scheme based on a Schwarz technique with overlapping subdomains, which converges ε-uniformly with respect to both the number of mesh points and the number of iterations. The step-size of such special meshes is extremely small in the neighborhood of the layer and changes sharply on its boundary, that (as was shown by A.A. Samarskii) can generally lead to a loss of well-conditioning of the above schemes. For the decomposition scheme we study the conditioning of the system (difference scheme) and the conditioning of the system matrix (difference operator), and also the influence of perturbations in the data of the boundary-value problem on disturbances of its numerical solutions. We derive estimates for the disturbances of the numerical solutions (in the maximum norm) depending on the subdomain in which the disturbance of the data appears. It is shown that the condition number of the difference operator associated with the Schwarz method, just as for the base scheme, is not ε-uniformly bounded. However, these difference schemes are well-conditioned ε-uniformly (with the ε-uniform estimate for the condition number being the same as for the schemes on uniform meshes for regular problems) when the right-hand side of the discrete equations is considered in a "natural” norm, i.e., in the maximum norm with a special weight multiplier. In the case of the boundary-value problem with perturbed data we give conditions under which the solution of the iterative scheme based on the overlapping Schwarz method is convergent ε-uniformly to the solution of this Dirichlet problem as the number of mesh points and the number of iterations increase. | |
| 540 | |a This article is distributed under the terms of the Creative Commons Attribution Non-Commercial License, which permits unrestricted non-commercial use, distribution, and reproduction in any medium, provided the original work is properly cited. | ||
| 690 | 7 | |a singular perturbation problem |2 nationallicence | |
| 690 | 7 | |a convection-diffusion equations |2 nationallicence | |
| 690 | 7 | |a ε-uniform fitted mesh method |2 nationallicence | |
| 690 | 7 | |a domain decomposition method |2 nationallicence | |
| 690 | 7 | |a condition numbers |2 nationallicence | |
| 773 | 0 | |t Computational Methods in Applied Mathematics |d De Gruyter |g 3/3(2003), 459-487 |x 1609-4840 |q 3:3<459 |1 2003 |2 3 |o cmam | |
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| 950 | |B NATIONALLICENCE |P 100 |E 1- |a Shishkin |D Gregorii I. |u Institute of Mathematics and Mechanics, Ural Branch of the Russian Academy of Sciences, 16 S. Kovalevskaya Str., 620219 Ekaterinburg, Russia | ||
| 950 | |B NATIONALLICENCE |P 773 |E 0- |t Computational Methods in Applied Mathematics |d De Gruyter |g 3/3(2003), 459-487 |x 1609-4840 |q 3:3<459 |1 2003 |2 3 |o cmam | ||
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