X-Git-Url: https://bilbo.iut-bm.univ-fcomte.fr/and/gitweb/hpcc2014.git/blobdiff_plain/f2d52a8e01117d631783d873860e90d32f2bf8d5..a091bb5ea8523eab4cda5bd035da309c347c95e5:/hpcc.tex?ds=sidebyside diff --git a/hpcc.tex b/hpcc.tex index 497ed68..c3a0b34 100644 --- a/hpcc.tex +++ b/hpcc.tex @@ -106,25 +106,25 @@ increasing complexity of these requested applications combined with a continuou distributed and parallel algorithms requiring significant hardware resources (grid computing, clusters, broadband network, etc.) but also a non-negligible CPU execution time. We consider in this paper a class of highly efficient parallel algorithms called \emph{numerical iterative algorithms} executed in a distributed environment. As their name -suggests, these algorithm solves a given problem by successive iterations ($X_{n +1} = f(X_{n})$) from an initial value +suggests, these algorithms solve a given problem by successive iterations ($X_{n +1} = f(X_{n})$) from an initial value $X_{0}$ to find an approximate value $X^*$ of the solution with a very low residual error. Several well-known methods -demonstrate the convergence of these algorithms \cite{BT89,Bahi07}. +demonstrate the convergence of these algorithms~\cite{BT89,Bahi07}. -Parallelization of such algorithms generally involved the division of the problem into several \emph{blocks} that will +Parallelization of such algorithms generally involve the division of the problem into several \emph{blocks} that will be solved in parallel on multiple processing units. The latter will communicate each intermediate results before a new iteration starts and until the approximate solution is reached. These parallel computations can be performed either in -\emph{synchronous} mode where a new iteration begin only when all nodes communications are completed, -either \emph{asynchronous} mode where processors can continue independently without or few synchronization points. For -instance in the \textit{Asynchronous Iterations~-- Asynchronous Communications (AIAC)} model \cite{bcvc06:ij}, local +\emph{synchronous} mode where a new iteration begins only when all nodes communications are completed, +or in \emph{asynchronous} mode where processors can continue independently with few or no synchronization points. For +instance in the \textit{Asynchronous Iterations~-- Asynchronous Communications (AIAC)} model~\cite{bcvc06:ij}, local computations do not need to wait for required data. Processors can then perform their iterations with the data present at that time. Even if the number of iterations required before the convergence is generally greater than for the synchronous case, AIAC algorithms can significantly reduce overall execution times by suppressing idle times due to -synchronizations especially in a grid computing context (see \cite{Bahi07} for more details). +synchronizations especially in a grid computing context (see~\cite{Bahi07} for more details). Parallel numerical applications (synchronous or asynchronous) may have different configuration and deployment requirements. Quantifying their resource allocation policies and application scheduling algorithms in grid computing environments under varying load, CPU power and network speeds is very costly, very labor intensive and very time -consuming \cite{Calheiros:2011:CTM:1951445.1951450}. The case of AIAC algorithms is even more problematic since they are very sensible to the +consuming~\cite{Calheiros:2011:CTM:1951445.1951450}. The case of AIAC algorithms is even more problematic since they are very sensible to the execution environment context. For instance, variations in the network bandwidth (intra and inter-clusters), in the number and the power of nodes, in the number of clusters... can lead to very different number of iterations and so to very different execution times. Then, it appears that the use of simulation tools to explore various platform @@ -138,14 +138,14 @@ best of execution time. To our knowledge, there is no existing work on the large-scale simulation of a real AIAC application. The aim of this paper is twofold. First we give a first approach of the simulation of AIAC algorithms using a simulation tool (i.e. the -SimGrid toolkit \cite{SimGrid}). Second, we confirm the effectiveness of asynchronous mode algorithms by comparing their +SimGrid toolkit~\cite{SimGrid}). Second, we confirm the effectiveness of asynchronous mode algorithms by comparing their performance with the synchronous mode. More precisely, we had implemented a program for solving large non-symmetric linear system of equations by numerical method GMRES (Generalized Minimal Residual) []. We show, that with minor modifications of the initial MPI code, the SimGrid toolkit allows us to perform a test campaign of a real AIAC application on different computing architectures. The simulated results we obtained are in line with real results -exposed in ??. SimGrid had allowed us to launch the application from a modest computing infrastructure by simulating -different distributed architectures composed by clusters nodes interconnected by variable speed networks. It has been -permitted to show With selected parameters on the network platforms (bandwidth, latency of inter cluster network) and +exposed in ??\AG[]{??}. SimGrid had allowed us to launch the application from a modest computing infrastructure by simulating +different distributed architectures composed by clusters nodes interconnected by variable speed networks. +With selected parameters on the network platforms (bandwidth, latency of inter cluster network) and on the clusters architecture (number, capacity calculation power) in the simulated environment, the experimental results have demonstrated not only the algorithm convergence within a reasonable time compared with the physical environment performance, but also a time saving of up to \np[\%]{40} in asynchronous mode. @@ -160,7 +160,7 @@ carried out will be presented before some concluding remarks and future works. As exposed in the introduction, parallel iterative methods are now widely used in many scientific domains. They can be classified in three main classes depending on how iterations and communications are managed (for more details readers -can refer to \cite{bcvc06:ij}). In the \textit{Synchronous Iterations~-- Synchronous Communications (SISC)} model data +can refer to~\cite{bcvc06:ij}). In the \textit{Synchronous Iterations~-- Synchronous Communications (SISC)} model data are exchanged at the end of each iteration. All the processors must begin the same iteration at the same time and important idle times on processors are generated. The \textit{Synchronous Iterations~-- Asynchronous Communications (SIAC)} model can be compared to the previous one except that data required on another processor are sent asynchronously @@ -169,10 +169,10 @@ but unfortunately, the overlapping is only partial and important idle times rema computing context, where the number of computational nodes is large, heterogeneous and widely distributed, the idle times generated by synchronizations are very penalizing. One way to overcome this problem is to use the \textit{Asynchronous Iterations~-- Asynchronous Communications (AIAC)} model. Here, local computations do not need to -wait for required data. Processors can then perform their iterations with the data present at that time. Figure -\ref{fig:aiac} illustrates this model where the gray blocks represent the computation phases, the white spaces the idle +wait for required data. Processors can then perform their iterations with the data present at that time. Figure~\ref{fig:aiac} +illustrates this model where the gray blocks represent the computation phases, the white spaces the idle times and the arrows the communications. With this algorithmic model, the number of iterations required before the -convergence is generally greater than for the two former classes. But, and as detailed in \cite{bcvc06:ij}, AIAC +convergence is generally greater than for the two former classes. But, and as detailed in~\cite{bcvc06:ij}, AIAC algorithms can significantly reduce overall execution times by suppressing idle times due to synchronizations especially in a grid computing context. @@ -202,7 +202,7 @@ iterations and so to very different execution times. \section{SimGrid} -SimGrid~\cite{casanova+legrand+quinson.2008.simgrid,SimGrid} is a simulation +SimGrid~\cite{SimGrid,casanova+legrand+quinson.2008.simgrid} is a simulation framework to study the behavior of large-scale distributed systems. As its name says, it emanates from the grid computing community, but is nowadays used to study grids, clouds, HPC or peer-to-peer systems. The early versions of SimGrid @@ -234,35 +234,36 @@ with little or no modifications. SMPI implements about \np[\%]{80} of the MPI \section{Simulation of the multisplitting method} %Décrire le problème (algo) traité ainsi que le processus d'adaptation à SimGrid. Let $Ax=b$ be a large sparse system of $n$ linear equations in $\mathbb{R}$, where $A$ is a sparse square and nonsingular matrix, $x$ is the solution vector and $b$ is the right-hand side vector. We use a multisplitting method based on the block Jacobi splitting to solve this linear system on a large scale platform composed of $L$ clusters of processors~\cite{o1985multi}. In this case, we apply a row-by-row splitting without overlapping -\[ -\left(\begin{array}{ccc} -A_{11} & \cdots & A_{1L} \\ -\vdots & \ddots & \vdots\\ -A_{L1} & \cdots & A_{LL} -\end{array} \right) -\times -\left(\begin{array}{c} -X_1 \\ -\vdots\\ -X_L -\end{array} \right) -= -\left(\begin{array}{c} -B_1 \\ -\vdots\\ -B_L -\end{array} \right)\] +\begin{equation*} + \left(\begin{array}{ccc} + A_{11} & \cdots & A_{1L} \\ + \vdots & \ddots & \vdots\\ + A_{L1} & \cdots & A_{LL} + \end{array} \right) + \times + \left(\begin{array}{c} + X_1 \\ + \vdots\\ + X_L + \end{array} \right) + = + \left(\begin{array}{c} + B_1 \\ + \vdots\\ + B_L + \end{array} \right) +\end{equation*} in such a way that successive rows of matrix $A$ and both vectors $x$ and $b$ are assigned to one cluster, where for all $l,m\in\{1,\ldots,L\}$ $A_{lm}$ is a rectangular block of $A$ of size $n_l\times n_m$, $X_l$ and $B_l$ are sub-vectors of $x$ and $b$, respectively, of size $n_l$ each and $\sum_{l} n_l=\sum_{m} n_m=n$. The multisplitting method proceeds by iteration to solve in parallel the linear system on $L$ clusters of processors, in such a way each sub-system \begin{equation} -\left\{ -\begin{array}{l} -A_{ll}X_l = Y_l \mbox{,~such that}\\ -Y_l = B_l - \displaystyle\sum_{\substack{m=1\\ m\neq l}}^{L}A_{lm}X_m -\end{array} -\right. -\label{eq:4.1} + \label{eq:4.1} + \left\{ + \begin{array}{l} + A_{ll}X_l = Y_l \text{, such that}\\ + Y_l = B_l - \displaystyle\sum_{\substack{m=1\\ m\neq l}}^{L}A_{lm}X_m + \end{array} + \right. \end{equation} is solved independently by a cluster and communications are required to update the right-hand side sub-vector $Y_l$, such that the sub-vectors $X_m$ represent the data dependencies between the clusters. As each sub-system (\ref{eq:4.1}) is solved in parallel by a cluster of processors, our multisplitting method uses an iterative method as an inner solver which is easier to parallelize and more scalable than a direct method. In this work, we use the parallel algorithm of GMRES method~\cite{ref1} which is one of the most used iterative method by many researchers. @@ -277,14 +278,17 @@ is solved independently by a cluster and communications are required to update t \For {$k=0,1,2,\ldots$ until the global convergence} \State Restart outer iteration with $x^0=x^k$ \State Inner iteration: \Call{InnerSolver}{$x^0$, $k+1$} -\State Send shared elements of $X_l^{k+1}$ to neighboring clusters -\State Receive shared elements in $\{X_m^{k+1}\}_{m\neq l}$ +\State\label{algo:01:send} Send shared elements of $X_l^{k+1}$ to neighboring clusters +\State\label{algo:01:recv} Receive shared elements in $\{X_m^{k+1}\}_{m\neq l}$ \EndFor \Statex \Function {InnerSolver}{$x^0$, $k$} -\State Compute local right-hand side $Y_l$: \[Y_l = B_l - \sum\nolimits^L_{\substack{m=1 \\m\neq l}}A_{lm}X_m^0\] +\State Compute local right-hand side $Y_l$: + \begin{equation*} + Y_l = B_l - \sum\nolimits^L_{\substack{m=1\\ m\neq l}}A_{lm}X_m^0 + \end{equation*} \State Solving sub-system $A_{ll}X_l^k=Y_l$ with the parallel GMRES method \State \Return $X_l^k$ \EndFunction @@ -303,9 +307,9 @@ $\{A_{lm}\}_{m\neq l}$ are off-diagonal matrices of sparse matrix $A$ and $\{X_m\}_{m\neq l}$ contain vector elements of solution $x$ shared with neighboring clusters. At every outer iteration $k$, asynchronous communications are performed between processors of the local cluster and those of distant -clusters (lines $6$ and $7$ in Figure~\ref{algo:01}). The shared vector -elements of the solution $x$ are exchanged by message passing using MPI -non-blocking communication routines. +clusters (lines~\ref{algo:01:send} and~\ref{algo:01:recv} in +Figure~\ref{algo:01}). The shared vector elements of the solution $x$ are +exchanged by message passing using MPI non-blocking communication routines. \begin{figure}[!t] \centering @@ -314,8 +318,24 @@ non-blocking communication routines. \label{fig:4.1} \end{figure} -The global convergence of the asynchronous multisplitting solver is detected when the clusters of processors have all converged locally. We implemented the global convergence detection process as follows. On each cluster a master processor is designated (for example the processor with rank $1$) and masters of all clusters are interconnected by a virtual unidirectional ring network (see Figure~\ref{fig:4.1}). During the resolution, a Boolean token circulates around the virtual ring from a master processor to another until the global convergence is achieved. So starting from the cluster with rank $1$, each master processor $i$ sets the token to {\it True} if the local convergence is achieved or to {\it False} otherwise, and sends it to master processor $i+1$. Finally, the global convergence is detected when the master of cluster $1$ receives from the master of cluster $L$ a token set to {\it True}. In this case, the master of cluster $1$ broadcasts a stop message to masters of other clusters. In this work, the local convergence on each cluster $l$ is detected when the following condition is satisfied -\[(k\leq \MI) \mbox{~or~} (\|X_l^k - X_l^{k+1}\|_{\infty}\leq\epsilon)\] +The global convergence of the asynchronous multisplitting solver is detected +when the clusters of processors have all converged locally. We implemented the +global convergence detection process as follows. On each cluster a master +processor is designated (for example the processor with rank 1) and masters of +all clusters are interconnected by a virtual unidirectional ring network (see +Figure~\ref{fig:4.1}). During the resolution, a Boolean token circulates around +the virtual ring from a master processor to another until the global convergence +is achieved. So starting from the cluster with rank 1, each master processor $i$ +sets the token to \textit{True} if the local convergence is achieved or to +\text\it{False} otherwise, and sends it to master processor $i+1$. Finally, the +global convergence is detected when the master of cluster 1 receives from the +master of cluster $L$ a token set to \textit{True}. In this case, the master of +cluster 1 broadcasts a stop message to masters of other clusters. In this work, +the local convergence on each cluster $l$ is detected when the following +condition is satisfied +\begin{equation*} + (k\leq \MI) \text{ or } (\|X_l^k - X_l^{k+1}\|_{\infty}\leq\epsilon) +\end{equation*} where $\MI$ is the maximum number of outer iterations and $\epsilon$ is the tolerance threshold of the error computed between two successive local solution $X_l^k$ and $X_l^{k+1}$. \LZK{Description du processus d'adaptation de l'algo multisplitting à SimGrid} @@ -346,39 +366,48 @@ results. When the \emph{real} application runs in the simulation environment and produces the expected results, varying the input parameters and the program arguments allows us to compare outputs from the code execution. We have noticed from this study that the results depend on the following parameters: -\begin{itemize} -\item At the network level, we found that -the most critical values are the bandwidth (bw) and the network latency (lat). -\item Hosts power (GFlops) can also -influence on the results. -\item Finally, when submitting job batches for execution, the arguments values passed to the -program like the maximum number of iterations or the \emph{external} precision are critical. They allow to ensure not -only the convergence of the algorithm but also to get the main objective of the experimentation of the simulation in -having an execution time in asynchronous less than in synchronous mode (i.e. speed-up less than $1$). +\begin{itemize} +\item At the network level, we found that the most critical values are the + bandwidth (bw) and the network latency (lat). +\item Hosts power (GFlops) can also influence on the results. +\item Finally, when submitting job batches for execution, the arguments values + passed to the program like the maximum number of iterations or the + \emph{external} precision are critical. They allow to ensure not only the + convergence of the algorithm but also to get the main objective of the + experimentation of the simulation in having an execution time in asynchronous + less than in synchronous mode (i.e. speed-up less than 1). \end{itemize} -A priori, obtaining a speedup less than $1$ would be difficult in a local area -network configuration where the synchronous mode will take advantage on the rapid -exchange of information on such high-speed links. Thus, the methodology adopted -was to launch the application on clustered network. In this last configuration, -degrading the inter-cluster network performance will \emph{penalize} the synchronous -mode allowing to get a speedup lower than $1$. This action simulates the case of -clusters linked with long distance network like Internet. +A priori, obtaining a speedup less than 1 would be difficult in a local area +network configuration where the synchronous mode will take advantage on the +rapid exchange of information on such high-speed links. Thus, the methodology +adopted was to launch the application on clustered network. In this last +configuration, degrading the inter-cluster network performance will +\emph{penalize} the synchronous mode allowing to get a speedup lower than 1. +This action simulates the case of clusters linked with long distance network +like Internet. As a first step, the algorithm was run on a network consisting of two clusters -containing $50$ hosts each, totaling $100$ hosts. Various combinations of -the above factors have providing the results shown in -Table~\ref{tab.cluster.2x50} with a matrix size ranging from $N_x = N_y = N_z = -62 \text{ to } 171$ elements or from $62^{3} = \np{238328}$ to $171^{3} = -\np{5211000}$ entries. +containing 50 hosts each, totaling 100 hosts. Various combinations of the above +factors have providing the results shown in Table~\ref{tab.cluster.2x50} with a +matrix size ranging from $N_x = N_y = N_z = \text{62}$ to 171 elements or from +$\text{62}^\text{3} = \text{\np{238328}}$ to $\text{171}^\text{3} = +\text{\np{5211000}}$ entries. + +% use the same column width for the following three tables +\newlength{\mytablew}\settowidth{\mytablew}{\footnotesize\np{E-11}} +\newenvironment{mytable}[1]{% #1: number of columns for data + \renewcommand{\arraystretch}{1.3}% + \begin{tabular}{|>{\bfseries}r% + |*{#1}{>{\centering\arraybackslash}p{\mytablew}|}}}{% + \end{tabular}} \begin{table}[!t] \centering - \caption{$2$ clusters, each with $50$ nodes} + \caption{2 clusters, each with 50 nodes} \label{tab.cluster.2x50} - \renewcommand{\arraystretch}{1.3} - \begin{tabular}{|>{\bfseries}r|*{12}{c|}} + \begin{mytable}{6} \hline bw & 5 & 5 & 5 & 5 & 5 & 50 \\ @@ -398,11 +427,11 @@ Table~\ref{tab.cluster.2x50} with a matrix size ranging from $N_x = N_y = N_z = speedup & 0.396 & 0.392 & 0.396 & 0.391 & 0.393 & 0.395 \\ \hline - \end{tabular} + \end{mytable} \smallskip - \begin{tabular}{|>{\bfseries}r|*{12}{c|}} + \begin{mytable}{6} \hline bw & 50 & 50 & 50 & 50 & 10 & 10 \\ @@ -422,22 +451,21 @@ Table~\ref{tab.cluster.2x50} with a matrix size ranging from $N_x = N_y = N_z = speedup & 0.398 & 0.388 & 0.393 & 0.394 & 0.63 & 0.778 \\ \hline - \end{tabular} + \end{mytable} \end{table} Then we have changed the network configuration using three clusters containing -respectively $33$, $33$ and $34$ hosts, or again by on hundred hosts for all the +respectively 33, 33 and 34 hosts, or again by on hundred hosts for all the clusters. In the same way as above, a judicious choice of key parameters has permitted to get the results in Table~\ref{tab.cluster.3x33} which shows the -speedups less than $1$ with a matrix size from $62$ to $100$ elements. +speedups less than 1 with a matrix size from 62 to 100 elements. \begin{table}[!t] \centering - \caption{$3$ clusters, each with $33$ nodes} + \caption{3 clusters, each with 33 nodes} \label{tab.cluster.3x33} - \renewcommand{\arraystretch}{1.3} - \begin{tabular}{|>{\bfseries}r|*{6}{c|}} + \begin{mytable}{6} \hline bw & 10 & 5 & 4 & 3 & 2 & 6 \\ @@ -457,10 +485,9 @@ speedups less than $1$ with a matrix size from $62$ to $100$ elements. speedup & 0.997 & 0.99 & 0.93 & 0.84 & 0.78 & 0.99 \\ \hline - \end{tabular} + \end{mytable} \end{table} - In a final step, results of an execution attempt to scale up the three clustered configuration but increasing by two hundreds hosts has been recorded in Table~\ref{tab.cluster.3x67}. @@ -469,9 +496,8 @@ Table~\ref{tab.cluster.3x67}. \centering \caption{3 clusters, each with 66 nodes} \label{tab.cluster.3x67} - \renewcommand{\arraystretch}{1.3} - \begin{tabular}{|>{\bfseries}r|c|} + \begin{mytable}{1} \hline bw & 1 \\ \hline @@ -485,7 +511,7 @@ Table~\ref{tab.cluster.3x67}. \hline speedup & 0.9 \\ \hline - \end{tabular} + \end{mytable} \end{table} Note that the program was run with the following parameters: @@ -525,21 +551,21 @@ bandwidth, a latency in order of a hundredth of a millisecond and a system power of one GFlops, an efficiency of about \np[\%]{40} in asynchronous mode is obtained for a matrix size of 62 elements. It is noticed that the result remains stable even if we vary the external precision from \np{E-5} to \np{E-9}. By -increasing the problem size up to $100$ elements, it was necessary to increase the +increasing the problem size up to 100 elements, it was necessary to increase the CPU power of \np[\%]{50} to \np[GFlops]{1.5} for a convergence of the algorithm with the same order of asynchronous mode efficiency. Maintaining such a system power but this time, increasing network throughput inter cluster up to \np[Mbit/s]{50}, the result of efficiency of about \np[\%]{40} is obtained with -high external precision of \np{E-11} for a matrix size from $110$ to $150$ side +high external precision of \np{E-11} for a matrix size from 110 to 150 side elements. -For the $3$ clusters architecture including a total of 100 hosts, +For the 3 clusters architecture including a total of 100 hosts, Table~\ref{tab.cluster.3x33} shows that it was difficult to have a combination which gives an efficiency of asynchronous below \np[\%]{80}. Indeed, for a -matrix size of $62$ elements, equality between the performance of the two modes +matrix size of 62 elements, equality between the performance of the two modes (synchronous and asynchronous) is achieved with an inter cluster of \np[Mbit/s]{10} and a latency of \np[ms]{E-1}. To challenge an efficiency by -\np[\%]{78} with a matrix size of $100$ points, it was necessary to degrade the +\np[\%]{78} with a matrix size of 100 points, it was necessary to degrade the inter cluster network bandwidth from 5 to \np[Mbit/s]{2}. A last attempt was made for a configuration of three clusters but more powerful