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Non-Galerkin Coarse Grids for Algebraic Multigrid
Author(s) -
Robert D. Falgout,
Jacob B. Schroder
Publication year - 2014
Publication title -
siam journal on scientific computing
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.674
H-Index - 147
eISSN - 1095-7197
pISSN - 1064-8275
DOI - 10.1137/130931539
Subject(s) - stencil , multigrid method , mathematics , grid , discretization , galerkin method , operator (biology) , partial differential equation , discontinuous galerkin method , solver , finite element method , mathematical optimization , computational science , mathematical analysis , geometry , physics , thermodynamics , biochemistry , chemistry , repressor , gene , transcription factor
Algebraic multigrid (AMG) is a popular and effective solver for systems of linear equations that arise from discretized partial differential equations. While AMG has been effectively implemented on large scale parallel machines, challenges remain, especially when moving to exascale. In particular, stencil sizes (the number of nonzeros in a row) tend to increase further down in the coarse grid hierarchy, and this growth leads to more communication. Thus, as problem size increases and the number of levels in the hierarchy grows, the overall efficiency of the parallel AMG method decreases, sometimes dramatically. This growth in stencil size is due to the standard Galerkin coarse grid operator, $P^T A P$, where $P$ is the prolongation (i.e., interpolation) operator. For example, the coarse grid stencil size for a simple three-dimensional (3D) seven-point finite differencing approximation to diffusion can increase into the thousands on present day machines, causing an associated increase in communication costs...

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