X-Git-Url: https://bilbo.iut-bm.univ-fcomte.fr/and/gitweb/GMRES2stage.git/blobdiff_plain/9deeb3b22421122e2872c4c432662811ec125909..fd0a7d17543c653d442bccd0c7ee035764e83650:/paper.tex diff --git a/paper.tex b/paper.tex index e4421cd..e23ccc2 100644 --- a/paper.tex +++ b/paper.tex @@ -546,13 +546,14 @@ Iterative Krylov methods; sparse linear systems; error minimization; PETSc; %à % no \IEEEPARstart % You must have at least 2 lines in the paragraph with the drop letter % (should never be an issue) -{\bf RAPH : EST ce qu'on parle de Krylov pour dire que les résidus constituent une base de Krylov... J'hésite... Tof t'en penses quoi?} -Iterative methods are become more attractive than direct ones to solve very -large sparse linear systems. They are more effective in a parallel context and -require less memory and arithmetic operations than direct methods. A number of -iterative methods are proposed and adapted by many researchers and the increased -need for solving very large sparse linear systems triggered the development of -efficient iterative techniques suitable for the parallel processing. + +Iterative methods became more attractive than direct ones to solve very large +sparse linear systems. Iterative methods are more effecient in a parallel +context, with thousands of cores, and require less memory and arithmetic +operations than direct methods. A number of iterative methods are proposed and +adapted by many researchers and the increased need for solving very large sparse +linear systems triggered the development of efficient iterative techniques +suitable for the parallel processing. Most of the successful iterative methods currently available are based on Krylov subspaces which consist in forming a basis of a sequence of successive matrix @@ -574,15 +575,18 @@ large clusters. In this paper we propose a two-stage algorithm based on two nested iterations called inner-outer iterations. This algorithm consists in solving the sparse linear system iteratively with a small number of inner iterations and restarts -the outer step with a new solution minimizing some error functions over a Krylov -subspace. This algorithm is iterative and easy to parallelize on large clusters -and the minimization technique improves its convergence and performances. +the outer step with a new solution minimizing some error functions over some +previous residuals. This algorithm is iterative and easy to parallelize on large +clusters and the minimization technique improves its convergence and +performances. The present paper is organized as follows. In Section~\ref{sec:02} some related -works are presented. Section~\ref{sec:03} presents our two-stage algorithm based -on Krylov subspace iteration methods. Section~\ref{sec:04} shows some +works are presented. Section~\ref{sec:03} presents our two-stage algorithm using +a least-square residual minimization. Section~\ref{sec:04} describes some +convergence results on this method. Section~\ref{sec:05} shows some experimental results obtained on large clusters of our algorithm using routines -of PETSc toolkit. +of PETSc toolkit. Finally Section~\ref{sec:06} concludes and gives some +perspectives. %%%********************************************************* %%%********************************************************* @@ -665,12 +669,13 @@ reused with the new values of the residuals. %%%********************************************************* %%%********************************************************* - +\section{Convergence results} +\label{sec:04} %%%********************************************************* %%%********************************************************* \section{Experiments using petsc} -\label{sec:04} +\label{sec:05} In order to see the influence of our algorithm with only one processor, we first @@ -679,7 +684,7 @@ table~\ref{tab:01}, we show the matrices we have used and some of them characteristics. For all the matrices, the name, the field, the number of rows and the number of nonzero elements is given. -\begin{table} +\begin{table*} \begin{center} \begin{tabular}{|c|c|r|r|r|} \hline @@ -696,7 +701,7 @@ torso3 & 2D/3D problem & 259,156 & 4,429,042 \\ \caption{Main characteristics of the sparse matrices chosen from the Davis collection} \label{tab:01} \end{center} -\end{table} +\end{table*} The following parameters have been chosen for our experiments. As by default the restart of GMRES is performed every 30 iterations, we have chosen to stop @@ -783,6 +788,10 @@ Larger experiments .... nb. cores & threshold & \multicolumn{2}{c|}{gmres variant} & \multicolumn{2}{c|}{2 stage CGLS} & \multicolumn{2}{c|}{2 stage LSQR} & best gain \\ \cline{3-8} & & Time & \# Iter. & Time & \# Iter. & Time & \# Iter. & \\\hline \hline + 2,048 & 8e-5 & 108.88 & 16,560 & 23.06 & 3,630 & 22.79 & 3,630 & 4.77 \\ + 2,048 & 6e-5 & 194.01 & 30,270 & 35.50 & 5,430 & 27.74 & 4,350 & 6.99 \\ + 4,096 & 7e-5 & 160.59 & 22,530 & 35.15 & 5,130 & 29.21 & 4,350 & 5.49 \\ + 4,096 & 6e-5 & 249.27 & 35,520 & 52.13 & 7,950 & 39.24 & 5,790 & 6.35 \\ 8,192 & 6e-5 & 149.54 & 17,280 & 28.68 & 3,810 & 29.05 & 3,990 & 5.21 \\ 8,192 & 5e-5 & 792.11 & 109,590 & 76.83 & 10,470 & 65.20 & 9,030 & 12.14 \\ 16,384 & 4e-5 & 718.61 & 86,400 & 98.98 & 10,830 & 131.86 & 14,790 & 7.26 \\ @@ -801,7 +810,7 @@ Larger experiments .... %%%********************************************************* %%%********************************************************* \section{Conclusion} -\label{sec:05} +\label{sec:06} %The conclusion goes here. this is more of the conclusion %%%********************************************************* %%%*********************************************************