Title of program: ILUCG2 (Incomplete LU factorized Con-being stiff and requiring implicit solution techniques. Generjugate Gradient algorithm for 2D problems) ally, the resulting matrix equations are asymmetric; we solve them here with the ILUCG2 program. In a subsequent article Catalogue number: AC
ICCG2: Subprograms for the solution of a linear symmetric matrix equation arising from a 9-point discretization
β Scribed by D.V. Anderson; A.I. Shestakov
- Publisher
- Elsevier Science
- Year
- 1983
- Tongue
- English
- Weight
- 477 KB
- Volume
- 30
- Category
- Article
- ISSN
- 0010-4655
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β¦ Synopsis
Title ofprogram: ICCG2 (Incomplete Cholesky factorized Con-being stiff and requiring implicit solution techniques. Somejugate Gradient algorithm for 2D symmetric problems) times, the resulting matrix equations are symmetric; we solve them here with the ICCG2 coding. In a previous article we Catalogue number: ACEV described a slower more general algorithm, ILUCG2, which must be used when the matrix is asymmetric [4].
π SIMILAR VOLUMES
Title of program: ICCG3 (Incomplete Cholesky factorized Con-treated by similar methods in two dimensions using the codes jugate Gradient algorithm for 3D symmetric problems) ICCG2 [4] and ILUCG2 [5]. These problems share the common feature of being stiff and requiring implicit solution Catalogue num
## Nature of the physical problem Certain elliptic and parabolic partial differential equations that arise in plasma physics and other applications are solved in two dimensions. The implicit solution techniques used for these equations give rise to a system of linear equations whose matrix operato
A computer program written in FORTRAN IV for obtaining smooth solutions of ill-posed systems of linear equations arising from the discretization of the Fredholm integral equation of the first kind is given. It is based on a novel algorithm by the author. The algorithm is iterative using linear progr
## Abstract In this paper we consider a quadrature method for the solution of the doubleβlayer potential equation corresponding to Laplace's equation in a polygonal domain. We prove the stability for our method in case of special triangulations over the boundary of the polygon. For the solution of