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49 \title{Simulation of Asynchronous Iterative Algorithms Using SimGrid}
53 Charles Emile Ramamonjisoa\IEEEauthorrefmark{1},
54 Lilia Ziane Khodja\IEEEauthorrefmark{2},
55 David Laiymani\IEEEauthorrefmark{1},
56 Arnaud Giersch\IEEEauthorrefmark{1} and
57 Raphaël Couturier\IEEEauthorrefmark{1}
59 \IEEEauthorblockA{\IEEEauthorrefmark{1}%
60 Femto-ST Institute -- DISC Department\\
61 Université de Franche-Comté,
62 IUT de Belfort-Montbéliard\\
63 19 avenue du Maréchal Juin, BP 527, 90016 Belfort cedex, France\\
64 Email: \email{{charles.ramamonjisoa,david.laiymani,arnaud.giersch,raphael.couturier}@univ-fcomte.fr}
66 \IEEEauthorblockA{\IEEEauthorrefmark{2}%
67 Inria Bordeaux Sud-Ouest\\
68 200 avenue de la Vieille Tour, 33405 Talence cedex, France \\
69 Email: \email{lilia.ziane@inria.fr}
77 Synchronous iterative algorithms are often less scalable than asynchronous
78 iterative ones. Performing large scale experiments with different kind of
79 network parameters is not easy because with supercomputers such parameters are
80 fixed. So one solution consists in using simulations first in order to analyze
81 what parameters could influence or not the behaviors of an algorithm. In this
82 paper, we show that it is interesting to use SimGrid to simulate the behaviors
83 of asynchronous iterative algorithms. For that, we compare the behaviour of a
84 synchronous GMRES algorithm with an asynchronous multisplitting one with
85 simulations in which we choose some parameters. Both codes are real MPI
86 codes. Simulations allow us to see when the multisplitting algorithm can be more
87 efficient than the GMRES one to solve a 3D Poisson problem.
90 % no keywords for IEEE conferences
91 % Keywords: Algorithm distributed iterative asynchronous simulation SimGrid
94 \section{Introduction}
96 Parallel computing and high performance computing (HPC) are becoming more and more imperative for solving various
97 problems raised by researchers on various scientific disciplines but also by industrial in the field. Indeed, the
98 increasing complexity of these requested applications combined with a continuous increase of their sizes lead to write
99 distributed and parallel algorithms requiring significant hardware resources (grid computing, clusters, broadband
100 network, etc.) but also a non-negligible CPU execution time. We consider in this paper a class of highly efficient
101 parallel algorithms called \emph{iterative algorithms} executed in a distributed environment. As their name
102 suggests, these algorithms solve a given problem by successive iterations ($X_{n +1} = f(X_{n})$) from an initial value
103 $X_{0}$ to find an approximate value $X^*$ of the solution with a very low residual error. Several well-known methods
104 demonstrate the convergence of these algorithms~\cite{BT89,Bahi07}.
106 Parallelization of such algorithms generally involve the division of the problem
107 into several \emph{blocks} that will be solved in parallel on multiple
108 processing units. The latter will communicate each intermediate results before a
109 new iteration starts and until the approximate solution is reached. These
110 parallel computations can be performed either in \emph{synchronous} mode where a
111 new iteration begins only when all nodes communications are completed, or in
112 \emph{asynchronous} mode where processors can continue independently with no
113 synchronization points~\cite{bcvc06:ij}. In this case, local computations do not
114 need to wait for required data. Processors can then perform their iterations
115 with the data present at that time. Even if the number of iterations required
116 before the convergence is generally greater than for the synchronous case,
117 asynchronous iterative algorithms can significantly reduce overall execution
118 times by suppressing idle times due to synchronizations especially in a grid
119 computing context (see~\cite{Bahi07} for more details).
121 Parallel applications based on a (synchronous or asynchronous) iteration model
122 may have different configuration and deployment requirements. Quantifying their
123 resource allocation policies and application scheduling algorithms in grid
124 computing environments under varying load, CPU power and network speeds is very
125 costly, very labor intensive and very time
126 consuming~\cite{Calheiros:2011:CTM:1951445.1951450}. The case of asynchronous
127 iterative algorithms is even more problematic since they are very sensible to
128 the execution environment context. For instance, variations in the network
129 bandwidth (intra and inter-clusters), in the number and the power of nodes, in
130 the number of clusters\dots{} can lead to very different number of iterations
131 and so to very different execution times. Then, it appears that the use of
132 simulation tools to explore various platform scenarios and to run large numbers
133 of experiments quickly can be very promising. In this way, the use of a
134 simulation environment to execute parallel iterative algorithms found some
135 interests in reducing the highly cost of access to computing resources: (1) for
136 the applications development life cycle and in code debugging (2) and in
137 production to get results in a reasonable execution time with a simulated
138 infrastructure not accessible with physical resources. Indeed, the launch of
139 distributed iterative asynchronous algorithms to solve a given problem on a
140 large-scale simulated environment challenges to find optimal configurations
141 giving the best results with a lowest residual error and in the best of
145 To our knowledge, there is no existing work on the large-scale simulation of a
146 real asynchronous iterative application. {\bf The contribution of the present
147 paper can be summarised in two main points}. First we give a first approach
148 of the simulation of asynchronous iterative algorithms using a simulation tool
149 (i.e. the SimGrid toolkit~\cite{SimGrid}). Second, we confirm the
150 effectiveness of the asynchronous multisplitting algorithm by comparing its
151 performance with the synchronous GMRES (Generalized Minimal Residual)
152 \cite{ref1}. Both these codes can be used to solve large linear systems. In
153 this paper, we focus on a 3D Poisson problem. We show, that with minor
154 modifications of the initial MPI code, the SimGrid toolkit allows us to perform
155 a test campaign of a real asynchronous iterative application on different
156 computing architectures.
157 % The simulated results we
158 %obtained are in line with real results exposed in ??\AG[]{ref?}.
159 SimGrid had allowed us to launch the application from a modest computing
160 infrastructure by simulating different distributed architectures composed by
161 clusters nodes interconnected by variable speed networks. Parameters of the
162 network platforms are the bandwidth and the latency of inter cluster
163 network. Parameters on the cluster's architecture are the number of machines and
164 the computation power of a machine. Simulations show that the asynchronous
165 multisplitting algorithm can solve the 3D Poisson problem approximately twice
166 faster than GMRES with two distant clusters.
170 This article is structured as follows: after this introduction, the next section
171 will give a brief description of iterative asynchronous model. Then, the
172 simulation framework SimGrid is presented with the settings to create various
173 distributed architectures. Then, the multisplitting method is presented, it is
174 based on GMRES to solve each block obtained of the splitting. This code is
175 written with MPI primitives and its adaptation to SimGrid with SMPI (Simulated
176 MPI) is detailed in the next section. At last, the simulation results carried
177 out will be presented before some concluding remarks and future works.
180 \section{Motivations and scientific context}
182 As exposed in the introduction, parallel iterative methods are now widely used
183 in many scientific domains. They can be classified in three main classes
184 depending on how iterations and communications are managed (for more details
185 readers can refer to~\cite{bcvc06:ij}). In the synchronous iterations model,
186 data are exchanged at the end of each iteration. All the processors must begin
187 the same iteration at the same time and important idle times on processors are
188 generated. It is possible to use asynchronous communications, in this case, the
189 model can be compared to the previous one except that data required on another
190 processor are sent asynchronously i.e. without stopping current computations.
191 This technique allows to partially overlap communications by computations but
192 unfortunately, the overlapping is only partial and important idle times remain.
193 It is clear that, in a grid computing context, where the number of computational
194 nodes is large, heterogeneous and widely distributed, the idle times generated
195 by synchronizations are very penalizing. One way to overcome this problem is to
196 use the asynchronous iterations model. Here, local computations do not need to
197 wait for required data. Processors can then perform their iterations with the
198 data present at that time. Figure~\ref{fig:aiac} illustrates this model where
199 the gray blocks represent the computation phases. With this algorithmic model,
200 the number of iterations required before the convergence is generally greater
201 than for the two former classes. But, and as detailed in~\cite{bcvc06:ij},
202 asynchronous iterative algorithms can significantly reduce overall execution
203 times by suppressing idle times due to synchronizations especially in a grid
208 \includegraphics[width=8cm]{AIAC.pdf}
209 \caption{The asynchronous iterations model}
214 %% It is very challenging to develop efficient applications for large scale,
215 %% heterogeneous and distributed platforms such as computing grids. Researchers and
216 %% engineers have to develop techniques for maximizing application performance of
217 %% these multi-cluster platforms, by redesigning the applications and/or by using
218 %% novel algorithms that can account for the composite and heterogeneous nature of
219 %% the platform. Unfortunately, the deployment of such applications on these very
220 %% large scale systems is very costly, labor intensive and time consuming. In this
221 %% context, it appears that the use of simulation tools to explore various platform
222 %% scenarios at will and to run enormous numbers of experiments quickly can be very
223 %% promising. Several works\dots{}
225 %% \AG{Several works\dots{} what?\\
226 % Le paragraphe suivant se trouve déjà dans l'intro ?}
227 In the context of asynchronous algorithms, the number of iterations to reach the
228 convergence depends on the delay of messages. With synchronous iterations, the
229 number of iterations is exactly the same than in the sequential mode (if the
230 parallelization process does not change the algorithm). So the difficulty with
231 asynchronous iteratie algorithms comes from the fact it is necessary to run the algorithm
232 with real data. In fact, from an execution to another the order of messages will
233 change and the number of iterations to reach the convergence will also change.
234 According to all the parameters of the platform (number of nodes, power of
235 nodes, inter and intra clusrters bandwith and latency, ....) and of the
236 algorithm (number of splitting with the multisplitting algorithm), the
237 multisplitting code will obtain the solution more or less quickly. Or course,
238 the GMRES method also depends of the same parameters. As it is difficult to have
239 access to many clusters, grids or supercomputers with many different network
240 parameters, it is interesting to be able to simulate the behaviors of
241 asynchronous iterative algoritms before being able to runs real experiments.
250 SimGrid~\cite{SimGrid,casanova+legrand+quinson.2008.simgrid} is a simulation
251 framework to study the behavior of large-scale distributed systems. As its name
252 says, it emanates from the grid computing community, but is nowadays used to
253 study grids, clouds, HPC or peer-to-peer systems. The early versions of SimGrid
254 date from 1999, but it's still actively developed and distributed as an open
255 source software. Today, it's one of the major generic tools in the field of
256 simulation for large-scale distributed systems.
258 SimGrid provides several programming interfaces: MSG to simulate Concurrent
259 Sequential Processes, SimDAG to simulate DAGs of (parallel) tasks, and SMPI to
260 run real applications written in MPI~\cite{MPI}. Apart from the native C
261 interface, SimGrid provides bindings for the C++, Java, Lua and Ruby programming
262 languages. SMPI is the interface that has been used for the work exposed in
263 this paper. The SMPI interface implements about \np[\%]{80} of the MPI 2.0
264 standard~\cite{bedaride:hal-00919507}, and supports applications written in C or
265 Fortran, with little or no modifications.
267 Within SimGrid, the execution of a distributed application is simulated on a
268 single machine. The application code is really executed, but some operations
269 like the communications are intercepted, and their running time is computed
270 according to the characteristics of the simulated execution platform. The
271 description of this target platform is given as an input for the execution, by
272 the mean of an XML file. It describes the properties of the platform, such as
273 the computing nodes with their computing power, the interconnection links with
274 their bandwidth and latency, and the routing strategy. The simulated running
275 time of the application is computed according to these properties.
277 To compute the durations of the operations in the simulated world, and to take
278 into account resource sharing (e.g. bandwidth sharing between competing
279 communications), SimGrid uses a fluid model. This allows to run relatively fast
280 simulations, while still keeping accurate
281 results~\cite{bedaride:hal-00919507,tomacs13}. Moreover, depending on the
282 simulated application, SimGrid/SMPI allows to skip long lasting computations and
283 to only take their duration into account. When the real computations cannot be
284 skipped, but the results have no importance for the simulation results, there is
285 also the possibility to share dynamically allocated data structures between
286 several simulated processes, and thus to reduce the whole memory consumption.
287 These two techniques can help to run simulations at a very large scale.
289 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
290 \section{Simulation of the multisplitting method}
292 \subsection{The multisplitting method}
293 %Décrire le problème (algo) traité ainsi que le processus d'adaptation à SimGrid.
294 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
296 \left(\begin{array}{ccc}
297 A_{11} & \cdots & A_{1L} \\
298 \vdots & \ddots & \vdots\\
299 A_{L1} & \cdots & A_{LL}
302 \left(\begin{array}{c}
308 \left(\begin{array}{c}
314 in such a way that successive rows of matrix $A$ and both vectors $x$ and $b$
315 are assigned to one cluster, where for all $\ell,m\in\{1,\ldots,L\}$, $A_{\ell
316 m}$ is a rectangular block of $A$ of size $n_\ell\times n_m$, $X_\ell$ and
317 $B_\ell$ are sub-vectors of $x$ and $b$, respectively, of size $n_\ell$ each,
318 and $\sum_{\ell} n_\ell=\sum_{m} n_m=n$.
320 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
325 A_{\ell\ell}X_\ell = Y_\ell \text{, such that}\\
326 Y_\ell = B_\ell - \displaystyle\sum_{\substack{m=1\\ m\neq \ell}}^{L}A_{\ell m}X_m
330 is solved independently by a cluster and communications are required to update
331 the right-hand side sub-vector $Y_\ell$, such that the sub-vectors $X_m$
332 represent the data dependencies between the clusters. As each sub-system
333 (\ref{eq:4.1}) is solved in parallel by a cluster of processors, our
334 multisplitting method uses an iterative method as an inner solver which is
335 easier to parallelize and more scalable than a direct method. In this work, we
336 use the parallel algorithm of GMRES method~\cite{ref1} which is one of the most
337 used iterative method by many researchers.
340 %%% IEEE instructions forbid to use an algorithm environment here, use figure
342 \begin{algorithmic}[1]
343 \Input $A_\ell$ (sparse sub-matrix), $B_\ell$ (right-hand side sub-vector)
344 \Output $X_\ell$ (solution sub-vector)\medskip
346 \State Load $A_\ell$, $B_\ell$
347 \State Set the initial guess $x^0$
348 \For {$k=0,1,2,\ldots$ until the global convergence}
349 \State Restart outer iteration with $x^0=x^k$
350 \State Inner iteration: \Call{InnerSolver}{$x^0$, $k+1$}
351 \State\label{algo:01:send} Send shared elements of $X_\ell^{k+1}$ to neighboring clusters
352 \State\label{algo:01:recv} Receive shared elements in $\{X_m^{k+1}\}_{m\neq \ell}$
357 \Function {InnerSolver}{$x^0$, $k$}
358 \State Compute local right-hand side $Y_\ell$:
360 Y_\ell = B_\ell - \sum\nolimits^L_{\substack{m=1\\ m\neq \ell}}A_{\ell m}X_m^0
362 \State Solving sub-system $A_{\ell\ell}X_\ell^k=Y_\ell$ with the parallel GMRES method
363 \State \Return $X_\ell^k$
366 \caption{A multisplitting solver with GMRES method}
370 Algorithm on Figure~\ref{algo:01} shows the main key points of the
371 multisplitting method to solve a large sparse linear system. This algorithm is
372 based on an outer-inner iteration method where the parallel synchronous GMRES
373 method is used to solve the inner iteration. It is executed in parallel by each
374 cluster of processors. For all $\ell,m\in\{1,\ldots,L\}$, the matrices and
375 vectors with the subscript $\ell$ represent the local data for cluster $\ell$,
376 while $\{A_{\ell m}\}_{m\neq \ell}$ are off-diagonal matrices of sparse matrix
377 $A$ and $\{X_m\}_{m\neq \ell}$ contain vector elements of solution $x$ shared
378 with neighboring clusters. At every outer iteration $k$, asynchronous
379 communications are performed between processors of the local cluster and those
380 of distant clusters (lines~\ref{algo:01:send} and~\ref{algo:01:recv} in
381 Figure~\ref{algo:01}). The shared vector elements of the solution $x$ are
382 exchanged by message passing using MPI non-blocking communication routines.
386 \includegraphics[width=60mm,keepaspectratio]{clustering}
387 \caption{Example of three clusters of processors interconnected by a virtual unidirectional ring network.}
391 The global convergence of the asynchronous multisplitting solver is detected
392 when the clusters of processors have all converged locally. We implemented the
393 global convergence detection process as follows. On each cluster a master
394 processor is designated (for example the processor with rank 1) and masters of
395 all clusters are interconnected by a virtual unidirectional ring network (see
396 Figure~\ref{fig:4.1}). During the resolution, a Boolean token circulates around
397 the virtual ring from a master processor to another until the global convergence
398 is achieved. So starting from the cluster with rank 1, each master processor $i$
399 sets the token to \textit{True} if the local convergence is achieved or to
400 \textit{False} otherwise, and sends it to master processor $i+1$. Finally, the
401 global convergence is detected when the master of cluster 1 receives from the
402 master of cluster $L$ a token set to \textit{True}. In this case, the master of
403 cluster 1 broadcasts a stop message to masters of other clusters. In this work,
404 the local convergence on each cluster $\ell$ is detected when the following
405 condition is satisfied
407 (k\leq \MI) \text{ or } (\|X_\ell^k - X_\ell^{k+1}\|_{\infty}\leq\epsilon)
409 where $\MI$ is the maximum number of outer iterations and $\epsilon$ is the
410 tolerance threshold of the error computed between two successive local solution
411 $X_\ell^k$ and $X_\ell^{k+1}$.
415 In this paper, we solve the 3D Poisson problem whose the mathematical model is
419 \nabla^2 u = f \text{~in~} \Omega \\
420 u =0 \text{~on~} \Gamma =\partial\Omega
425 where $\nabla^2$ is the Laplace operator, $f$ and $u$ are real-valued functions, and $\Omega=[0,1]^3$. The spatial discretization with a finite difference scheme reduces problem~(\ref{eq:02}) to a system of sparse linear equations. Our multisplitting method solves the 3D Poisson problem using a seven point stencil whose the general expression could be written as
428 u(x-1,y,z) + u(x,y-1,z) + u(x,y,z-1)\\+u(x+1,y,z)+u(x,y+1,z)+u(x,y,z+1) \\ -6u(x,y,z)=h^2f(x,y,z),
429 %u(x,y,z)= & \frac{1}{6}\times [u(x-1,y,z) + u(x+1,y,z) + \\
430 % & u(x,y-1,z) + u(x,y+1,z) + \\
431 % & u(x,y,z-1) + u(x,y,z+1) - \\ & h^2f(x,y,z)],
435 where $h$ is the distance between two adjacent elements in the spatial discretization scheme and the iteration matrix $A$ of size $N_x\times N_y\times N_z$ of the discretized linear system is sparse, symmetric and positive definite.
437 The parallel solving of the 3D Poisson problem with our multisplitting method requires a data partitioning of the problem between clusters and between processors within a cluster. We have chosen the 3D partitioning instead of the row-by-row partitioning in order to reduce the data exchanges at sub-domain boundaries. Figure~\ref{fig:4.2} shows an example of the data partitioning of the 3D Poisson problem between two clusters of processors, where each sub-problem is assigned to a processor. In this context, a processor has at most six neighbors within a cluster or in distant clusters with which it shares data at sub-domain boundaries.
441 \includegraphics[width=80mm,keepaspectratio]{partition}
442 \caption{Example of the 3D data partitioning between two clusters of processors.}
447 \subsection{Simulation of the multisplitting method using SimGrid and SMPI}
451 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
452 We did not encounter major blocking problems when adapting the multisplitting algorithm previously described to a simulation environment like SimGrid unless some code
453 debugging. Indeed, apart from the review of the program sequence for asynchronous exchanges between processors within a cluster or between clusters, the algorithm was executed successfully with SMPI and provided identical outputs as those obtained with direct execution under MPI. In synchronous
454 mode, the execution of the program raised no particular issue but in asynchronous mode, the review of the sequence of MPI\_Isend, MPI\_Irecv and MPI\_Waitall instructions
455 and with the addition of the primitive MPI\_Test was needed to avoid a memory fault due to an infinite loop resulting from the non-convergence of the algorithm.
456 %\CER{On voulait en fait montrer la simplicité de l'adaptation de l'algo a SimGrid. Les problèmes rencontrés décrits dans ce paragraphe concerne surtout le mode async}\LZK{OK. J'aurais préféré avoir un peu plus de détails sur l'adaptation de la version async}
457 %\CER{Le problème majeur sur l'adaptation MPI vers SMPI pour la partie asynchrone de l'algorithme a été le plantage en SMPI de Waitall après un Isend et Irecv. J'avais proposé un workaround en utilisant un MPI\_wait séparé pour chaque échange a la place d'un waitall unique pour TOUTES les échanges, une instruction qui semble bien fonctionner en MPI. Ce workaround aussi fonctionne bien. Mais après, tu as modifié le programme avec l'ajout d'un MPI\_Test, au niveau de la routine de détection de la convergence et du coup, l'échange global avec waitall a aussi fonctionné.}
458 Note here that the use of SMPI functions optimizer for memory footprint and CPU usage is not recommended knowing that one wants to get real results by simulation.
459 As mentioned, upon this adaptation, the algorithm is executed as in the real life in the simulated environment after the following minor changes. The scope of all declared
460 global variables have been moved to local to subroutine. Indeed, global variables generate side effects arising from the concurrent access of
461 shared memory used by threads simulating each computing unit in the SimGrid architecture.
462 %Second, some compilation errors on MPI\_Waitall and MPI\_Finalize primitives have been fixed with the latest version of SimGrid.
463 %\AG{compilation or run-time error?}
464 In total, the initial MPI program running on the simulation environment SMPI gave after a very simple adaptation the same results as those obtained in a real
465 environment. We have successfully executed the code in synchronous mode using parallel GMRES algorithm compared with our multisplitting algorithm in asynchronous mode after few modifications.
469 \section{Simulation results}
471 When the \textit{real} application runs in the simulation environment and produces the expected results, varying the input
472 parameters and the program arguments allows us to compare outputs from the code execution. We have noticed from this
473 study that the results depend on the following parameters:
475 \item At the network level, we found that the most critical values are the
476 bandwidth and the network latency.
477 \item Hosts processors power (GFlops) can also influence on the results.
478 \item Finally, when submitting job batches for execution, the arguments values
479 passed to the program like the maximum number of iterations or the precision are critical. They allow us to ensure not only the convergence of the
480 algorithm but also to get the main objective in getting an execution time in asynchronous communication less than in
481 synchronous mode. The ratio between the simulated execution time of synchronous GMRES algorithm
482 compared to the asynchronous multisplitting algorithm ($t_\text{GMRES} / t_\text{Multisplitting}$) is defined as the \emph{relative gain}. So,
483 our objective running the algorithm in SimGrid is to obtain a relative gain
487 A priori, obtaining a relative gain greater than 1 would be difficult in a local
488 area network configuration where the synchronous mode will take advantage on the
489 rapid exchange of information on such high-speed links. Thus, the methodology
490 adopted was to launch the application on a clustered network. In this
491 configuration, degrading the inter-cluster network performance will penalize the
492 synchronous mode allowing to get a relative gain greater than 1. This action
493 simulates the case of distant clusters linked with long distance network as in grid computing context.
497 Both codes were simulated on a two clusters based network with 50 hosts each, totaling 100 hosts. Various combinations of the above
498 factors have provided the results shown in Table~\ref{tab.cluster.2x50}. The problem size of the 3D Poisson problem ranges from $N_x = N_y = N_z = \text{62}$ to 150 elements (that is from
499 $\text{62}^\text{3} = \text{\np{238328}}$ to $\text{150}^\text{3} =
500 \text{\np{3375000}}$ entries). With the asynchronous multisplitting algorithm the simulated execution time is in average 2.5 times faster than with the synchronous GMRES one.
501 %\AG{Expliquer comment lire les tableaux.}
502 %\CER{J'ai reformulé la phrase par la lecture du tableau. Plus de détails seront lus dans la partie Interprétations et commentaires}
503 % use the same column width for the following three tables
504 \newlength{\mytablew}\settowidth{\mytablew}{\footnotesize\np{E-11}}
505 \newenvironment{mytable}[1]{% #1: number of columns for data
506 \renewcommand{\arraystretch}{1.3}%
507 \begin{tabular}{|>{\bfseries}r%
508 |*{#1}{>{\centering\arraybackslash}p{\mytablew}|}}}{%
513 \caption{2 clusters, each with 50 nodes}
514 \label{tab.cluster.2x50}
519 & 5 & 5 & 5 & 5 & 5 \\
522 & 0.02 & 0.02 & 0.02 & 0.02 & 0.02 \\
525 & 1 & 1 & 1 & 1.5 & 1.5 \\
528 & 62 & 62 & 62 & 100 & 100 \\
531 & \np{E-5} & \np{E-8} & \np{E-9} & \np{E-11} & \np{E-11} \\
535 & 2.52 & 2.55 & 2.52 & 2.57 & 2.54 \\
544 & 50 & 50 & 50 & 50 & 50 \\ % & 10 & 10 \\
547 & 0.02 & 0.02 & 0.02 & 0.02 & 0.02 \\ % & 0.03 & 0.01 \\
550 & 1.5 & 1.5 & 1.5 & 1.5 & 1.5 \\ % & 1 & 1.5 \\
553 & 110 & 120 & 130 & 140 & 150 \\ % & 171 & 171 \\
556 & \np{E-11} & \np{E-11} & \np{E-11} & \np{E-11} & \np{E-11} \\ % & \np{E-5} & \np{E-5} \\
560 & 2.53 & 2.51 & 2.58 & 2.55 & 2.54 \\ % & 1.59 & 1.29 \\
565 %Then we have changed the network configuration using three clusters containing
566 %respectively 33, 33 and 34 hosts, or again by on hundred hosts for all the
567 %clusters. In the same way as above, a judicious choice of key parameters has
568 %permitted to get the results in Table~\ref{tab.cluster.3x33} which shows the
569 %relative gains greater than 1 with a matrix size from 62 to 100 elements.
571 \CER{En accord avec RC, on a pour le moment enlevé les tableaux 2 et 3 sachant que les résultats obtenus sont limites. De même, on a enlevé aussi les deux dernières colonnes du tableau I en attendant une meilleure performance et une meilleure precision}
574 % \caption{3 clusters, each with 33 nodes}
575 % \label{tab.cluster.3x33}
580 % & 10 & 5 & 4 & 3 & 2 & 6 \\
583 % & 0.01 & 0.02 & 0.02 & 0.02 & 0.02 & 0.02 \\
586 % & 1 & 1 & 1 & 1 & 1 & 1 \\
589 % & 62 & 100 & 100 & 100 & 100 & 171 \\
592 % & \np{E-5} & \np{E-5} & \np{E-5} & \np{E-5} & \np{E-5} & \np{E-5} \\
596 % & 1.003 & 1.01 & 1.08 & 1.19 & 1.28 & 1.01 \\
601 %In a final step, results of an execution attempt to scale up the three clustered
602 %configuration but increasing by two hundreds hosts has been recorded in
603 %Table~\ref{tab.cluster.3x67}.
607 % \caption{3 clusters, each with 66 nodes}
608 % \label{tab.cluster.3x67}
620 % Prec/Eprec & \np{E-5} \\
623 % Relative gain & 1.11 \\
628 Note that the program was run with the following parameters:
630 \paragraph*{SMPI parameters}
633 \item HOSTFILE: Text file containing the list of the processors units name. Here 100 hosts;
634 \item PLATFORM: XML file description of the platform architecture whith the following characteristics: %two clusters (cluster1 and cluster2) with the following characteristics :
636 \item 2 clusters of 50 hosts each;
637 \item Processor unit power: \np[GFlops]{1.5};
638 \item Intracluster network bandwidth: \np[Gbit/s]{1.25} and latency:
640 \item Intercluster network bandwidth: \np[Mbit/s]{5} and latency:
646 \paragraph*{Arguments of the program}
649 \item Description of the cluster architecture matching the format <Number of
650 clusters> <Number of hosts in cluster1> <Number of hosts in cluster2>;
651 \item Maximum number of iterations;
652 \item Precisions on the residual error;
653 \item Matrix size $N_x$, $N_y$ and $N_z$;
654 \item Matrix diagonal value: $6$ (See Equation~(\ref{eq:03}));
655 \item Matrix off-diagonal value: $-1$;
656 \item Communication mode: asynchronous.
659 \paragraph*{Interpretations and comments}
661 After analyzing the outputs, generally, for the two clusters including one hundred hosts configuration (Tables~\ref{tab.cluster.2x50}), some combinations of parameters affecting
662 the results have given a relative gain more than 2.5, showing the effectiveness of the
663 asynchronous performance compared to the synchronous mode.
665 With these settings, Table~\ref{tab.cluster.2x50} shows
666 that after a deterioration of inter cluster network with a bandwidth of \np[Mbit/s]{5} and a latency in order of one hundredth of millisecond and a processor power
667 of one GFlops, an efficiency of about \np[\%]{40} is
668 obtained in asynchronous mode for a matrix size of 62 elements. It is noticed that the result remains
669 stable even we vary the residual error precision from \np{E-5} to \np{E-9}. By
670 increasing the matrix size up to 100 elements, it was necessary to increase the
671 CPU power of \np[\%]{50} to \np[GFlops]{1.5} to get the algorithm convergence and the same order of asynchronous mode efficiency. Maintaining such processor power but increasing network throughput inter cluster up to
672 \np[Mbit/s]{50}, the result of efficiency with a relative gain of 2.5 is obtained with
673 high external precision of \np{E-11} for a matrix size from 110 to 150 side
676 %For the 3 clusters architecture including a total of 100 hosts,
677 %Table~\ref{tab.cluster.3x33} shows that it was difficult to have a combination
678 %which gives a relative gain of asynchronous mode more than 1.2. Indeed, for a
679 %matrix size of 62 elements, equality between the performance of the two modes
680 %(synchronous and asynchronous) is achieved with an inter cluster of
681 %\np[Mbit/s]{10} and a latency of \np[ms]{E-1}. To challenge an efficiency greater than 1.2 with a matrix %size of 100 points, it was necessary to degrade the
682 %inter cluster network bandwidth from 5 to \np[Mbit/s]{2}.
683 \AG{Conclusion, on prend une plateforme pourrie pour avoir un bon ratio sync/async ???
684 Quelle est la perte de perfs en faisant ça ?}
686 %A last attempt was made for a configuration of three clusters but more powerful
687 %with 200 nodes in total. The convergence with a relative gain around 1.1 was
688 %obtained with a bandwidth of \np[Mbit/s]{1} as shown in
689 %Table~\ref{tab.cluster.3x67}.
691 %\RC{Est ce qu'on sait expliquer pourquoi il y a une telle différence entre les résultats avec 2 et 3 clusters... Avec 3 clusters, ils sont pas très bons... Je me demande s'il ne faut pas les enlever...}
692 %\RC{En fait je pense avoir la réponse à ma remarque... On voit avec les 2 clusters que le gain est d'autant plus grand qu'on choisit une bonne précision. Donc, plusieurs solutions, lancer rapidement un long test pour confirmer ca, ou enlever des tests... ou on ne change rien :-)}
693 %\LZK{Ma question est: le bandwidth et latency sont ceux inter-clusters ou pour les deux inter et intra cluster??}
694 %\CER{Définitivement, les paramètres réseaux variables ici se rapportent au réseau INTER cluster.}
696 The experimental results on executing a parallel iterative algorithm in
697 asynchronous mode on an environment simulating a large scale of virtual
698 computers organized with interconnected clusters have been presented.
699 Our work has demonstrated that using such a simulation tool allow us to
700 reach the following three objectives:
703 \item To have a flexible configurable execution platform resolving the
704 hard exercise to access to very limited but so solicited physical
706 \item to ensure the algorithm convergence with a reasonable time and
708 \item and finally and more importantly, to find the correct combination
709 of the cluster and network specifications permitting to save time in
710 executing the algorithm in asynchronous mode.
712 Our results have shown that in certain conditions, asynchronous mode is
713 speeder up to \np[\%]{40} than executing the algorithm in synchronous mode
714 which is not negligible for solving complex practical problems with more
715 and more increasing size.
717 Several studies have already addressed the performance execution time of
718 this class of algorithm. The work presented in this paper has
719 demonstrated an original solution to optimize the use of a simulation
720 tool to run efficiently an iterative parallel algorithm in asynchronous
721 mode in a grid architecture.
723 \LZK{Perspectives???}
725 \section*{Acknowledgment}
727 This work is partially funded by the Labex ACTION program (contract ANR-11-LABX-01-01).
728 \todo[inline]{The authors would like to thank\dots{}}
730 % trigger a \newpage just before the given reference
731 % number - used to balance the columns on the last page
732 % adjust value as needed - may need to be readjusted if
733 % the document is modified later
734 \bibliographystyle{IEEEtran}
735 \bibliography{IEEEabrv,hpccBib}
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748 % LocalWords: Ramamonjisoa Laiymani Arnaud Giersch Ziane Khodja Raphaël Femto
749 % LocalWords: Université Franche Comté IUT Montbéliard Maréchal Juin Inria Sud
750 % LocalWords: Ouest Vieille Talence cedex scalability experimentations HPC MPI
751 % LocalWords: Parallelization AIAC GMRES multi SMPI SISC SIAC SimDAG DAGs Lua
752 % LocalWords: Fortran GFlops priori Mbit de du fcomte multisplitting scalable
753 % LocalWords: SimGrid Belfort parallelize Labex ANR LABX IEEEabrv hpccBib
754 % LocalWords: intra durations nonsingular Waitall discretization discretized
755 % LocalWords: InnerSolver Isend Irecv