From 54896ac3f1c5c17afacb020e878a87e6303c8a37 Mon Sep 17 00:00:00 2001 From: David Laiymani Date: Wed, 6 May 2015 14:32:16 +0200 Subject: [PATCH] petites modifs intro --- paper.tex | 42 +++++++++++++++++++++--------------------- 1 file changed, 21 insertions(+), 21 deletions(-) diff --git a/paper.tex b/paper.tex index f1f47bf..25bf4d1 100644 --- a/paper.tex +++ b/paper.tex @@ -114,7 +114,7 @@ their applications using a simulation tool before. \end{abstract} %\keywords{Algorithm; distributed; iterative; asynchronous; simulation; simgrid; -%performance} +%performance} \keywords{ Performance evaluation, Simulation, SimGrid, Synchronous and asynchronous iterations, Multisplitting algorithms} \maketitle @@ -131,28 +131,28 @@ are often very important. So, in this context it is difficult to optimize a given application for a given architecture. In this way and in order to reduce the access cost to these computing resources it seems very interesting to use a simulation environment. The advantages are numerous: development life cycle, -code debugging, ability to obtain results quickly,~\ldots. In counterpart, the simulation results need to be consistent with the real ones. +code debugging, ability to obtain results quickly~\ldots. In counterpart, the simulation results need to be consistent with the real ones. In this paper we focus on a class of highly efficient parallel algorithms called \emph{iterative algorithms}. The parallel scheme of iterative methods is quite simple. It generally involves the division of the problem into several \emph{blocks} that will be solved in parallel on multiple processing -units. Each processing unit has to compute an iteration, to send/receive some +units. Each processing unit has to compute an iteration to send/receive some data dependencies to/from its neighbors and to iterate this process until the -convergence of the method. Several well-known methods demonstrate the +convergence of the method. Several well-known studies demonstrate the convergence of these algorithms~\cite{BT89,bahi07}. In this processing mode a task cannot begin a new iteration while it has not received data dependencies -from its neighbors. We say that the iteration computation follows a synchronous -scheme. In the asynchronous scheme a task can compute a new iteration without -having to wait for the data dependencies coming from its neighbors. Both -communication and computations are asynchronous inducing that there is no more -idle time, due to synchronizations, between two iterations~\cite{bcvc06:ij}. -This model presents some advantages and drawbacks that we detail in -section~\ref{sec:asynchro} but even if the number of iterations required to -converge is generally greater than for the synchronous case, it appears that -the asynchronous iterative scheme can significantly reduce overall execution -times by suppressing idle times due to synchronizations~(see~\cite{bahi07} -for more details). +from its neighbors. We say that the iteration computation follows a +\textit{synchronous} scheme. In the asynchronous scheme a task can compute a new +iteration without having to wait for the data dependencies coming from its +neighbors. Both communication and computations are \textit{asynchronous} +inducing that there is no more idle time, due to synchronizations, between two +iterations~\cite{bcvc06:ij}. This model presents some advantages and drawbacks +that we detail in section~\ref{sec:asynchro} but even if the number of +iterations required to converge is generally greater than for the synchronous +case, it appears that the asynchronous iterative scheme can significantly +reduce overall execution times by suppressing idle times due to +synchronizations~(see~\cite{bahi07} for more details). Nevertheless, in both cases (synchronous or asynchronous) it is very time consuming to find optimal configuration and deployment requirements for a given @@ -264,7 +264,7 @@ In this paper, we propose two algorithms of two-stage multisplitting methods. Th k\geq\MIM\mbox{~or~}\|x_\ell^{k+1}-x_\ell^k\|_{\infty }\leq\TOLM, \label{eq:04} \end{equation} -where $\MIM$ is the maximum number of outer iterations and $\TOLM$ is the tolerance threshold for the two-stage algorithm. +where $\MIM$ is the maximum number of outer iterations and $\TOLM$ is the tolerance threshold for the two-stage algorithm. The second two-stage algorithm is based on synchronous outer iterations. We propose to use the Krylov iteration based on residual minimization to improve the slow convergence of the multisplitting methods. In this case, a $n\times s$ matrix $S$ is set using solutions issued from the inner iteration \begin{equation} @@ -354,7 +354,7 @@ In addition, the following arguments are given to the programs at runtime: \item execution mode: synchronous or asynchronous; \RCE {C'est ok la liste des arguments du programme mais si Lilia ou toi pouvez preciser pour les arguments pour CGLS ci dessous} \RC{Vu que tu n'as pas fait varier ce paramètre, on peut ne pas en parler} \item Size of matrix S; - \item Maximum number of iterations and tolerance threshold for CGLS. + \item Maximum number of iterations and tolerance threshold for CGLS. \end{itemize} It should also be noticed that both solvers have been executed with the Simgrid selector -cfg=smpi/running\_power which determines the computational power (here 19GFlops) of the simulator host machine. @@ -379,16 +379,16 @@ such that \begin{equation*} \phi(x,y,z)=0\mbox{~on the boundary~}\partial\Omega \end{equation*} -where the real-valued function $\phi(x,y,z)$ is the solution sought, $f(x,y,z)$ is a known function and $\Omega=[0,1]^3$. The 3D discretization of the Laplace operator $\nabla^2$ with the finite difference scheme includes 7 points stencil on the computational grid. The numerical approximation of the Poisson problem on three-dimensional grid is repeatedly computed as $\phi=\phi^\star$ such that +where the real-valued function $\phi(x,y,z)$ is the solution sought, $f(x,y,z)$ is a known function and $\Omega=[0,1]^3$. The 3D discretization of the Laplace operator $\nabla^2$ with the finite difference scheme includes 7 points stencil on the computational grid. The numerical approximation of the Poisson problem on three-dimensional grid is repeatedly computed as $\phi=\phi^\star$ such that \begin{equation} \begin{array}{ll} \phi^\star(x,y,z)=&\frac{1}{6}(\phi(x-h,y,z)+\phi(x,y-h,z)+\phi(x,y,z-h)\\&+\phi(x+h,y,z)+\phi(x,y+h,z)+\phi(x,y,z+h)\\&-h^2f(x,y,z)) \end{array} \label{eq:08} \end{equation} -until convergence where $h$ is the grid spacing between two adjacent elements in the 3D computational grid. +until convergence where $h$ is the grid spacing between two adjacent elements in the 3D computational grid. -In the parallel context, the 3D Poisson problem is partitioned into $L\times p$ sub-problems such that $L$ is the number of clusters and $p$ is the number of processors in each cluster. We apply the three-dimensional partitioning instead of the row-by-row one in order to reduce the size of the data shared at the sub-problems boundaries. In this case, each processor is in charge of parallelepipedic block of the problem and has at most six neighbors in the same cluster or in distant clusters with which it shares data at boundaries. +In the parallel context, the 3D Poisson problem is partitioned into $L\times p$ sub-problems such that $L$ is the number of clusters and $p$ is the number of processors in each cluster. We apply the three-dimensional partitioning instead of the row-by-row one in order to reduce the size of the data shared at the sub-problems boundaries. In this case, each processor is in charge of parallelepipedic block of the problem and has at most six neighbors in the same cluster or in distant clusters with which it shares data at boundaries. \subsection{Study setup and Simulation Methodology} @@ -682,7 +682,7 @@ Using the Simgrid simulator flexibility, we have tried to determine the impact on the algorithms performance in varying the CPU power of the clusters nodes from 1 to 19 GFlops. The outputs depicted in the figure 6 confirm the performance gain, around 95\% for both of the two methods, -after adding more powerful CPU. +after adding more powerful CPU. \subsection{Comparing GMRES in native synchronous mode and Multisplitting algorithms in asynchronous mode} -- 2.39.5