ADI as a preconditioning for solving the convection diffusion equation

We examine a splitting of the operator obtained from a steady convection-diffusion equation with variable coefficients in which the convection term dominates. The operator is split into a dominant and a subdominant parts consistent with the inherent directional property of the partial differential e...

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Veröffentlicht in:SIAM J. Sci. Stat. Comput.; (United States) 1984-06, Vol.5 (2), p.281-299
Hauptverfasser: CHIN, R. C. Y, MANTEUFFEL, T. A, DE PILLIS, J
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Sprache:eng
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Zusammenfassung:We examine a splitting of the operator obtained from a steady convection-diffusion equation with variable coefficients in which the convection term dominates. The operator is split into a dominant and a subdominant parts consistent with the inherent directional property of the partial differential equation. The equations involving the dominant parts should be easily solved. We accelerate the convergence of this splitting or the outer iteration by a Chebyshev semi-iterative method. When the dominant part has constant coefficients, it can be easily solved using alternating direction implicit (ADI) methods. This is called the inner iteration. The optimal parameters for a stationary two-parameter ADI method are obtained when the eigenvalues become complex. This corresponds to either the horizontal or the vertical half-grid Reynolds number larger than unity. The Chebyshev semi-iterative method is used to accelerate the convergence of the inner ADI iteration. A two-fold increase in speed is obtained when the ADI iteration matrix has real eigenvalues, and the increase is less significant when the eigenvalues are complex. If either the horizontal or the vertical half-grid Reynolds number is equal to one, the spectral radius of the optimal ADI iterative matrix is zero. However, a high degree of nilpotency impairs rapid convergence. This problem is removed by introducing a more implicit iterative method called ADI/Gauss-Seidel (ADI/GS). ADI/GS resolves the nilpotency and, thus, converges more rapidly for half-grid Reynolds number near 1. Finally, our methods are compared with several well-known schemes on test problems.
ISSN:0196-5204
1064-8275
2168-3417
1095-7197
DOI:10.1137/0905020