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56 \title{Energy Consumption Reduction in a Heterogeneous Architecture Using DVFS}
67 University of Franche-Comté\\
68 IUT de Belfort-Montbéliard,
69 19 avenue du Maréchal Juin, BP 527, 90016 Belfort cedex, France\\
70 % Telephone: \mbox{+33 3 84 58 77 86}, % Raphaël
71 % Fax: \mbox{+33 3 84 58 77 81}\\ % Dept Info
72 Email: \email{{jean-claude.charr,raphael.couturier,ahmed.fanfakh_badri_muslim,arnaud.giersch}@univ-fcomte.fr}
79 Computing platforms are consuming more and more energy due to the increase of the number of nodes composing them. To minimize the operating costs of these platforms many techniques have been used. Dynamic voltage and frequency scaling (DVFS) is one of them, it reduces the frequency of a CPU to lower its energy consumption. However, lowering the frequency of a CPU might increase the execution time of an application running on that processor. Therefore, the frequency that gives the best tradeoff between the energy consumption and the performance of an application must be selected.
81 In this paper, a new online frequencies selecting algorithm for heterogeneous platforms is presented. It selects the frequency that gives the best tradeoff between energy saving and
82 performance degradation, for each node computing the message passing iterative application. The algorithm has a small overhead and works without training or profiling.
83 It uses a new energy model for message passing iterative applications running on a heterogeneous platform.
84 The proposed algorithm was evaluated on the Simgrid simulator while running the NAS parallel benchmarks.
85 The experiments demonstrated that it reduces the energy consumption up to 35\% while limiting the performance degradation as much as possible.
88 \section{Introduction}
90 The need for more computing power is continually increasing. To partially satisfy this need, most supercomputers constructors just put more computing nodes in their platform. The resulting platform might achieve higher floating point operations per second (FLOPS), but the energy consumption and the heat dissipation are also increased. As an example, the chinese supercomputer Tianhe-2 had the highest FLOPS in November 2014 according to the Top500 list \cite{TOP500_Supercomputers_Sites}. However, it was also the most power hungry platform with its over 3 millions cores consuming around 17.8 megawatts.
91 Moreover, according to the U.S. annual energy outlook 2014
92 \cite{U.S_Annual.Energy.Outlook.2014}, the price of energy for 1 megawatt-hour
93 was approximately equal to \$70.
94 Therefore, the price of the energy consumed by the
95 Tianhe-2 platform is approximately more than \$10 millions each year.
96 The computing platforms must be more energy efficient and offer the highest number of FLOPS per watt possible, such as the TSUBAME-KFC at the GSIC center of Tokyo which
97 became the top of the Green500 list in June 2014 \cite{Green500_List}.
98 This heterogeneous platform executes more than four GFLOPS per watt.
100 Besides hardware improvements, there are many software techniques to lower the energy consumption of these platforms, such as scheduling, DVFS, ... DVFS is a widely used process to reduce the energy
101 consumption of a processor by lowering its frequency. \textbf{put a reference to DVFS} However, it also the reduces the number of FLOPS executed by the processor which might increase the execution time of the application running over that processor.
102 Therefore, researchers used different optimization strategies to select the frequency that gives the best tradeoff between the energy reduction and
103 performance degradation ratio.
104 \textbf{you should talk about the first paper here and say that the algorithm was applied to a homogeneous platform then define what is a heterogeneous platform, you can take it from the firdt paragraph in section 3 }
106 In this paper, a frequency selecting algorithm is proposed. It selects the vector of frequencies for a heterogeneous platform that runs a message passing iterative application, that gives the maximum energy reduction and minimum
107 performance degradation ratio simultaneously. The algorithm has a very small
108 overhead, works online and does not need any training or profiling.
110 This paper is organized as follows: Section~\ref{sec.relwork} presents some
111 related works from other authors. Section~\ref{sec.exe} describes how the
112 execution time of message passing programs can be predicted. It also presents an energy
113 model that predicts the energy consumption of an application running over a heterogeneous platform. Section~\ref{sec.compet} presents
114 the energy-performance objective function that maximizes the reduction of energy
115 consumption while minimizing the degradation of the program's performance.
116 Section~\ref{sec.optim} details the proposed frequency selecting algorithm then the precision of the proposed algorithm is verified.\textbf{the verification should be put here}
117 Section~\ref{sec.expe} presents the results of applying the algorithm on the NAS parallel benchmarks and executing them
118 on a heterogeneous platform. It also shows the results of running three
119 different power scenarios and comparing them.
120 Finally, we conclude in Section~\ref{sec.concl} with a summary and some future works.
122 \textbf{never use we in an article and the algorithm is not heterogeneous! you cannot use scaling factors before defining what they are.}
123 \section{Related works}
125 DVFS is a technique enabled
126 in modern processors to scale down both the voltage and the frequency of
127 the CPU while computing, in order to reduce the energy consumption of the processor. DVFS is
128 also allowed in the GPUs to achieve the same goal. Reducing the frequency of a processor lowers its number of FLOPS and might degrade the performance of the application running on that processor, especially if it is compute bound. Therefore selecting the appropriate frequency for a processor to satisfy some objectives and while taking into account all the constraints, is not a trivial operation. Many researchers used different strategies to tackle this problem. Some of them used online methods that compute the new frequency while executing the application \textbf{add a reference for an online method here}. Others used offline methods that might need to run the application and profile it before selecting the new frequency \textbf{add a reference for an offline method}. The methods could be heuristics, exact or brute force methods that satisfy varied objectives such as energy reduction or performance. They also could be adapted to the execution's environment and the type of the application such as sequential, parallel or distributed architecture, homogeneous or heterogeneous platform, synchronous or asynchronous application, ...
130 In this paper, we are interested in reducing energy for message passing iterative synchronous applications running over heterogeneous platforms.
131 Some works have already been done for such platforms and it can be classified into two types of heterogeneous platforms:
134 \item the platform is composed of homogeneous GPUs and homogeneous CPUs.
135 \item the platform is only composed of heterogeneous CPUs.
139 For the first type of platform, the compute intensive parallel tasks are executed on the GPUs and the rest are executed
140 on the CPUs. Luley et al.
141 ~\cite{Luley_Energy.efficiency.evaluation.and.benchmarking}, proposed a heterogeneous
142 cluster composed of Intel Xeon CPUs and NVIDIA GPUs. Their main goal was to maximize the
143 energy efficiency of the platform during computation by maximizing the number of FLOPS per watt generated.
144 In~\cite{KaiMa_Holistic.Approach.to.Energy.Efficiency.in.GPU-CPU}, Kai Ma et al. developed a scheduling
145 algorithm that distributes workloads proportional to the computing power of the nodes which could be a GPU or a CPU. All the tasks must be completed at the same time.
146 In~\cite{Rong_Effects.of.DVFS.on.K20.GPU}, Rong et al. showed that
147 a heterogeneous (GPUs and CPUs) cluster that enables DVFS gave better energy and performance
148 efficiency than other clusters only composed of CPUs.
150 The work presented in this paper concerns the second type of platform,, with heterogeneous CPUs.
151 Many methods were conceived to reduce the energy consumption of this type of platform. Naveen et al.~\cite{Naveen_Power.Efficient.Resource.Scaling}
152 developed a method that minimize the value of $energy*delay^2$ by dynamically assigning new frequencies to the CPUs of the heterogeneous cluster. \textbf{should define the delay} Lizhe et al.~\cite{Lizhe_Energy.aware.parallel.task.scheduling} propose
153 an algorithm that divides the executed tasks into two types: the critical and
154 non critical tasks. The algorithm scales down the frequency of non critical tasks proportionally to their slack and communication times while limiting the performance degradation percentage to less than 10\%. In~\cite{Joshi_Blackbox.prediction.of.impact.of.DVFS}
155 and \cite{Spiliopoulos_Green.governors.Adaptive.DVFS}, a heterogeneous cluster composed of two types
156 of Intel and AMD processors. The consumed energy
157 and the performance for each frequency gear were predicted, then the algorithm selected the best gear that gave
158 the best tradeoff. \textbf{what energy model they used? what method they used? }
159 In~\cite{Shelepov_Scheduling.on.Heterogeneous.Multicore} and \cite{Li_Minimizing.Energy.Consumption.for.Frame.Based.Tasks},
160 the best frequencies for a specified heterogeneous cluster are selected offline using some
161 heuristic. Chen et al.~\cite{Chen_DVFS.under.quality.of.service.requirements} used a greedy dynamic approach to
162 minimize the power consumption of heterogeneous severs with time/space complexity \textbf{what does it mean}. This approach
163 had considerable overhead.
164 In contrast to the above described papers, this paper presents the following contributions :
166 \item two new energy and performance models for message passing iterative synchronous applications running over
167 a heterogeneous platform. Both models takes into account the communication and slack times. The models can predict the required energy and the execution time of the application.
169 \item a new online frequency selecting algorithm for heterogeneous platforms. The algorithm has a very small
170 overhead and does not need for any training or profiling. It uses a new optimization function which simultaneously maximizes the performance and minimizes the energy consumption of a message passing iterative synchronous application .
174 \section{The performance and energy consumption measurements on heterogeneous architecture}
177 % \JC{The whole subsection ``Parallel Tasks Execution on Homogeneous Platform'',
178 % can be deleted if we need space, we can just say we are interested in this
179 % paper in homogeneous clusters}
181 \subsection{The execution time of message passing distributed
182 iterative applications on a heterogeneous platform}
184 In this paper, we are interested in reducing the energy consumption of message
185 passing distributed iterative synchronous applications running over
186 heterogeneous platforms. We define a heterogeneous platform as a collection of
187 heterogeneous computing nodes interconnected via a high speed homogeneous
188 network. Therefore, each node has different characteristics such as computing
189 power (FLOPS), energy consumption, CPU's frequency range, \dots{} but they all
190 have the same network bandwidth and latency.
192 The overall execution time of a distributed iterative synchronous application
193 over a heterogeneous platform consists of the sum of the computation time and
194 the communication time for every iteration on a node. However, due to the
195 heterogeneous computation power of the computing nodes, slack times might occur
196 when fast nodes have to wait, during synchronous communications, for the slower
197 nodes to finish their computations (see Figure~(\ref{fig:heter})).
198 Therefore, the overall execution time of the program is the execution time of the slowest
199 task which have the highest computation time and no slack time.
203 \includegraphics[scale=0.6]{fig/commtasks}
204 \caption{Parallel tasks on a heterogeneous platform}
208 Dynamic Voltage and Frequency Scaling (DVFS) is a process, implemented in
209 modern processors, that reduces the energy consumption of a CPU by scaling
210 down its voltage and frequency. Since DVFS lowers the frequency of a CPU
211 and consequently its computing power, the execution time of a program running
212 over that scaled down processor might increase, especially if the program is
213 compute bound. The frequency reduction process can be expressed by the scaling
214 factor S which is the ratio between the maximum and the new frequency of a CPU
215 as in EQ (\ref{eq:s}).
218 S = \frac{F_\textit{max}}{F_\textit{new}}
220 The execution time of a compute bound sequential program is linearly proportional
221 to the frequency scaling factor $S$. On the other hand, message passing
222 distributed applications consist of two parts: computation and communication.
223 The execution time of the computation part is linearly proportional to the
224 frequency scaling factor $S$ but the communication time is not affected by the
225 scaling factor because the processors involved remain idle during the
226 communications~\cite{Freeh_Exploring.the.Energy.Time.Tradeoff}.
227 The communication time for a task is the summation of periods of
228 time that begin with an MPI call for sending or receiving a message
229 till the message is synchronously sent or received.
231 Since in a heterogeneous platform, each node has different characteristics,
232 especially different frequency gears, when applying DVFS operations on these
233 nodes, they may get different scaling factors represented by a scaling vector:
234 $(S_1, S_2,\dots, S_N)$ where $S_i$ is the scaling factor of processor $i$. To
235 be able to predict the execution time of message passing synchronous iterative
236 applications running over a heterogeneous platform, for different vectors of
237 scaling factors, the communication time and the computation time for all the
238 tasks must be measured during the first iteration before applying any DVFS
239 operation. Then the execution time for one iteration of the application with any
240 vector of scaling factors can be predicted using EQ (\ref{eq:perf}).
243 \textit T_\textit{new} =
244 \max_{i=1,2,\dots,N} ({TcpOld_{i}} \cdot S_{i}) + MinTcm
246 where $TcpOld_i$ is the computation time of processor $i$ during the first
247 iteration and $MinTcm$ is the communication time of the slowest processor from
248 the first iteration. The model computes the maximum computation time
249 with scaling factor from each node added to the communication time of the
250 slowest node, it means only the communication time without any slack time.
251 Therefore, we can consider the execution time of the iterative application is
252 equal to the execution time of one iteration as in EQ(\ref{eq:perf}) multiplied
253 by the number of iterations of that application.
255 This prediction model is developed from our model for predicting the execution time of
256 message passing distributed applications for homogeneous architectures~\cite{Our_first_paper}.
257 The execution time prediction model is used in our method for optimizing both
258 energy consumption and performance of iterative methods, which is presented in the
262 \subsection{Energy model for heterogeneous platform}
263 Many researchers~\cite{Malkowski_energy.efficient.high.performance.computing,
264 Rauber_Analytical.Modeling.for.Energy,Zhuo_Energy.efficient.Dynamic.Task.Scheduling,
265 Rizvandi_Some.Observations.on.Optimal.Frequency} divide the power consumed by a processor into
266 two power metrics: the static and the dynamic power. While the first one is
267 consumed as long as the computing unit is turned on, the latter is only consumed during
268 computation times. The dynamic power $Pd$ is related to the switching
269 activity $\alpha$, load capacitance $C_L$, the supply voltage $V$ and
270 operational frequency $F$, as shown in EQ(\ref{eq:pd}).
273 Pd = \alpha \cdot C_L \cdot V^2 \cdot F
275 The static power $Ps$ captures the leakage power as follows:
278 Ps = V \cdot N_{trans} \cdot K_{design} \cdot I_{leak}
280 where V is the supply voltage, $N_{trans}$ is the number of transistors,
281 $K_{design}$ is a design dependent parameter and $I_{leak}$ is a
282 technology-dependent parameter. The energy consumed by an individual processor
283 to execute a given program can be computed as:
286 E_\textit{ind} = Pd \cdot Tcp + Ps \cdot T
288 where $T$ is the execution time of the program, $Tcp$ is the computation
289 time and $Tcp \leq T$. $Tcp$ may be equal to $T$ if there is no
290 communication and no slack time.
292 The main objective of DVFS operation is to reduce the overall energy consumption~\cite{Le_DVFS.Laws.of.Diminishing.Returns}.
293 The operational frequency $F$ depends linearly on the supply voltage $V$, i.e., $V = \beta \cdot F$ with some
294 constant $\beta$. This equation is used to study the change of the dynamic
295 voltage with respect to various frequency values in~\cite{Rauber_Analytical.Modeling.for.Energy}. The reduction
296 process of the frequency can be expressed by the scaling factor $S$ which is the
297 ratio between the maximum and the new frequency as in EQ(\ref{eq:s}).
298 The CPU governors are power schemes supplied by the operating
299 system's kernel to lower a core's frequency. we can calculate the new frequency
300 $F_{new}$ from EQ(\ref{eq:s}) as follow:
303 F_\textit{new} = S^{-1} \cdot F_\textit{max}
305 Replacing $F_{new}$ in EQ(\ref{eq:pd}) as in EQ(\ref{eq:fnew}) gives the following
306 equation for dynamic power consumption:
309 {P}_\textit{dNew} = \alpha \cdot C_L \cdot V^2 \cdot F_{new} = \alpha \cdot C_L \cdot \beta^2 \cdot F_{new}^3 \\
310 {} = \alpha \cdot C_L \cdot V^2 \cdot F_{max} \cdot S^{-3} = P_{dOld} \cdot S^{-3}
312 where $ {P}_\textit{dNew}$ and $P_{dOld}$ are the dynamic power consumed with the
313 new frequency and the maximum frequency respectively.
315 According to EQ(\ref{eq:pdnew}) the dynamic power is reduced by a factor of $S^{-3}$ when
316 reducing the frequency by a factor of $S$~\cite{Rauber_Analytical.Modeling.for.Energy}. Since the FLOPS of a CPU is proportional
317 to the frequency of a CPU, the computation time is increased proportionally to $S$.
318 The new dynamic energy is the dynamic power multiplied by the new time of computation
319 and is given by the following equation:
322 E_\textit{dNew} = P_{dOld} \cdot S^{-3} \cdot (Tcp \cdot S)= S^{-2}\cdot P_{dOld} \cdot Tcp
324 The static power is related to the power leakage of the CPU and is consumed during computation
325 and even when idle. As in~\cite{Rauber_Analytical.Modeling.for.Energy,Zhuo_Energy.efficient.Dynamic.Task.Scheduling},
326 we assume that the static power of a processor is constant
327 during idle and computation periods, and for all its available frequencies.
328 The static energy is the static power multiplied by the execution time of the program.
329 According to the execution time model in EQ(\ref{eq:perf}), the execution time of the program
330 is the summation of the computation and the communication times. The computation time is linearly related
331 to the frequency scaling factor, while this scaling factor does not affect the communication time.
332 The static energy of a processor after scaling its frequency is computed as follows:
335 E_\textit{s} = Ps \cdot (Tcp \cdot S + Tcm)
338 In the considered heterogeneous platform, each processor $i$ might have different dynamic and
339 static powers, noted as $Pd_{i}$ and $Ps_{i}$ respectively. Therefore, even if the distributed
340 message passing iterative application is load balanced, the computation time of each CPU $i$
341 noted $Tcp_{i}$ might be different and different frequency scaling factors might be computed
342 in order to decrease the overall energy consumption of the application and reduce the slack times.
343 The communication time of a processor $i$ is noted as $Tcm_{i}$ and could contain slack times
344 if it is communicating with slower nodes, see figure(\ref{fig:heter}). Therefore, all nodes do
345 not have equal communication times. While the dynamic energy is computed according to the frequency
346 scaling factor and the dynamic power of each node as in EQ(\ref{eq:Edyn}), the static energy is
347 computed as the sum of the execution time of each processor multiplied by its static power.
348 The overall energy consumption of a message passing distributed application executed over a
349 heterogeneous platform during one iteration is the summation of all dynamic and static energies
350 for each processor. It is computed as follows:
353 E = \sum_{i=1}^{N} {(S_i^{-2} \cdot Pd_{i} \cdot Tcp_i)} + {} \\
354 \sum_{i=1}^{N} (Ps_{i} \cdot (\max_{i=1,2,\dots,N} (Tcp_i \cdot S_{i}) +
358 Reducing the frequencies of the processors according to the vector of
359 scaling factors $(S_1, S_2,\dots, S_N)$ may degrade the performance of the
360 application and thus, increase the static energy because the execution time is
361 increased~\cite{Kim_Leakage.Current.Moore.Law}. We can measure the overall energy consumption for the iterative
362 application by measuring the energy consumption for one iteration as in EQ(\ref{eq:energy})
363 multiplied by the number of iterations of that application.
366 \section{Optimization of both energy consumption and performance}
369 Using the lowest frequency for each processor does not necessarily gives the most energy
370 efficient execution of an application. Indeed, even though the dynamic power is reduced
371 while scaling down the frequency of a processor, its computation power is proportionally
372 decreased and thus the execution time might be drastically increased during which dynamic
373 and static powers are being consumed. Therefore, it might cancel any gains achieved by
374 scaling down the frequency of all nodes to the minimum and the overall energy consumption
375 of the application might not be the optimal one. It is not trivial to select the appropriate
376 frequency scaling factor for each processor while considering the characteristics of each processor
377 (computation power, range of frequencies, dynamic and static powers) and the task executed
378 (computation/communication ratio) in order to reduce the overall energy consumption and not
379 significantly increase the execution time. In our previous work~\cite{Our_first_paper}, we proposed a method
380 that selects the optimal frequency scaling factor for a homogeneous cluster executing a message
381 passing iterative synchronous application while giving the best trade-off between the energy
382 consumption and the performance for such applications. In this work we are interested in
383 heterogeneous clusters as described above. Due to the heterogeneity of the processors, not
384 one but a vector of scaling factors should be selected and it must give the best trade-off
385 between energy consumption and performance.
387 The relation between the energy consumption and the execution time for an application is
388 complex and nonlinear, Thus, unlike the relation between the execution time
389 and the scaling factor, the relation of the energy with the frequency scaling
390 factors is nonlinear, for more details refer to~\cite{Freeh_Exploring.the.Energy.Time.Tradeoff}.
391 Moreover, they are not measured using the same metric. To solve this problem, we normalize the
392 execution time by computing the ratio between the new execution time (after
393 scaling down the frequencies of some processors) and the initial one (with maximum
394 frequency for all nodes,) as follows:
397 P_\textit{Norm} = \frac{T_\textit{New}}{T_\textit{Old}}\\
398 {} = \frac{ \max_{i=1,2,\dots,N} (Tcp_{i} \cdot S_{i}) +MinTcm}
399 {\max_{i=1,2,\dots,N}{(Tcp_i+Tcm_i)}}
403 In the same way, we normalize the energy by computing the ratio between the consumed energy
404 while scaling down the frequency and the consumed energy with maximum frequency for all nodes:
407 E_\textit{Norm} = \frac{E_\textit{Reduced}}{E_\textit{Original}} \\
408 {} = \frac{ \sum_{i=1}^{N}{(S_i^{-2} \cdot Pd_i \cdot Tcp_i)} +
409 \sum_{i=1}^{N} {(Ps_i \cdot T_{New})}}{\sum_{i=1}^{N}{( Pd_i \cdot Tcp_i)} +
410 \sum_{i=1}^{N} {(Ps_i \cdot T_{Old})}}
412 Where $T_{New}$ and $T_{Old}$ are computed as in EQ(\ref{eq:pnorm}).
415 goal is to optimize the energy and execution time at the same time, the normalized
416 energy and execution time curves are not in the same direction. According
417 to the equations~(\ref{eq:enorm}) and~(\ref{eq:pnorm}), the vector of frequency
418 scaling factors $S_1,S_2,\dots,S_N$ reduce both the energy and the execution
419 time simultaneously. But the main objective is to produce maximum energy
420 reduction with minimum execution time reduction.
424 Our solution for this problem is to make the optimization process for energy and
425 execution time follow the same direction. Therefore, we inverse the equation of the
426 normalized execution time which gives the normalized performance equation, as follows:
429 P_\textit{Norm} = \frac{T_\textit{Old}}{T_\textit{New}}\\
430 = \frac{\max_{i=1,2,\dots,N}{(Tcp_i+Tcm_i)}}
431 { \max_{i=1,2,\dots,N} (Tcp_{i} \cdot S_{i}) + MinTcm}
437 \subfloat[Homogeneous platform]{%
438 \includegraphics[width=.22\textwidth]{fig/homo}\label{fig:r1}}%
440 \subfloat[Heterogeneous platform]{%
441 \includegraphics[width=.22\textwidth]{fig/heter}\label{fig:r2}}
443 \caption{The energy and performance relation}
446 Then, we can model our objective function as finding the maximum distance
447 between the energy curve EQ~(\ref{eq:enorm}) and the performance
448 curve EQ~(\ref{eq:pnorm_inv}) over all available sets of scaling factors. This
449 represents the minimum energy consumption with minimum execution time (maximum
450 performance) at the same time, see figure~(\ref{fig:r1}) or figure~(\ref{fig:r2}). Then our objective
451 function has the following form:
455 \max_{i=1,\dots F, j=1,\dots,N}
456 (\overbrace{P_\textit{Norm}(S_{ij})}^{\text{Maximize}} -
457 \overbrace{E_\textit{Norm}(S_{ij})}^{\text{Minimize}} )
459 where $N$ is the number of nodes and $F$ is the number of available frequencies for each nodes.
460 Then we can select the optimal set of scaling factors that satisfies EQ~(\ref{eq:max}).
461 Our objective function can work with any energy model or any power values for each node
462 (static and dynamic powers). However, the most energy reduction gain can be achieved when
463 the energy curve has a convex form as shown in~\cite{Zhuo_Energy.efficient.Dynamic.Task.Scheduling,Rauber_Analytical.Modeling.for.Energy,Hao_Learning.based.DVFS}.
465 \section{The scaling factors selection algorithm for heterogeneous platforms }
468 In this section we propose algorithm~(\ref{HSA}) which selects the frequency scaling factors
469 vector that gives the best trade-off between minimizing the energy consumption and maximizing
470 the performance of a message passing synchronous iterative application executed on a heterogeneous
471 platform. It works online during the execution time of the iterative message passing program.
472 It uses information gathered during the first iteration such as the computation time and the
473 communication time in one iteration for each node. The algorithm is executed after the first
474 iteration and returns a vector of optimal frequency scaling factors that satisfies the objective
475 function EQ(\ref{eq:max}). The program apply DVFS operations to change the frequencies of the CPUs
476 according to the computed scaling factors. This algorithm is called just once during the execution
477 of the program. Algorithm~(\ref{dvfs}) shows where and when the proposed scaling algorithm is called
478 in the iterative MPI program.
480 The nodes in a heterogeneous platform have different computing powers, thus while executing message
481 passing iterative synchronous applications, fast nodes have to wait for the slower ones to finish their
482 computations before being able to synchronously communicate with them as in figure (\ref{fig:heter}).
483 These periods are called idle or slack times.
484 Our algorithm takes into account this problem and tries to reduce these slack times when selecting the
485 frequency scaling factors vector. At first, it selects initial frequency scaling factors that increase
486 the execution times of fast nodes and minimize the differences between the computation times of
487 fast and slow nodes. The value of the initial frequency scaling factor for each node is inversely
488 proportional to its computation time that was gathered from the first iteration. These initial frequency
489 scaling factors are computed as a ratio between the computation time of the slowest node and the
490 computation time of the node $i$ as follows:
493 Scp_{i} = \frac{\max_{i=1,2,\dots,N}(Tcp_i)}{Tcp_i}
495 Using the initial frequency scaling factors computed in EQ(\ref{eq:Scp}), the algorithm computes
496 the initial frequencies for all nodes as a ratio between the maximum frequency of node $i$
497 and the computation scaling factor $Scp_i$ as follows:
500 F_{i} = \frac{Fmax_i}{Scp_i},~{i=1,2,\cdots,N}
502 If the computed initial frequency for a node is not available in the gears of that node, the computed
503 initial frequency is replaced by the nearest available frequency. In figure (\ref{fig:st_freq}),
504 the nodes are sorted by their computing powers in ascending order and the frequencies of the faster
505 nodes are scaled down according to the computed initial frequency scaling factors. The resulting new
506 frequencies are colored in blue in figure (\ref{fig:st_freq}). This set of frequencies can be considered
507 as a higher bound for the search space of the optimal vector of frequencies because selecting frequency
508 scaling factors higher than the higher bound will not improve the performance of the application and
509 it will increase its overall energy consumption. Therefore the algorithm that selects the frequency
510 scaling factors starts the search method from these initial frequencies and takes a downward search direction
511 toward lower frequencies. The algorithm iterates on all left frequencies, from the higher bound until all
512 nodes reach their minimum frequencies, to compute their overall energy consumption and performance, and select
513 the optimal frequency scaling factors vector. At each iteration the algorithm determines the slowest node
514 according to EQ(\ref{eq:perf}) and keeps its frequency unchanged, while it lowers the frequency of
515 all other nodes by one gear.
516 The new overall energy consumption and execution time are computed according to the new scaling factors.
517 The optimal set of frequency scaling factors is the set that gives the highest distance according to the objective
518 function EQ(\ref{eq:max}).
520 The plots~(\ref{fig:r1} and \ref{fig:r2}) illustrate the normalized performance and consumed energy for an
521 application running on a homogeneous platform and a heterogeneous platform respectively while increasing the
522 scaling factors. It can be noticed that in a homogeneous platform the search for the optimal scaling factor
523 should be started from the maximum frequency because the performance and the consumed energy is decreased since
524 the beginning of the plot. On the other hand, in the heterogeneous platform the performance is maintained at
525 the beginning of the plot even if the frequencies of the faster nodes are decreased until the scaled down nodes
526 have computing powers lower than the slowest node. In other words, until they reach the higher bound. It can
527 also be noticed that the higher the difference between the faster nodes and the slower nodes is, the bigger
528 the maximum distance between the energy curve and the performance curve is while varying the scaling factors
529 which results in bigger energy savings.
532 \includegraphics[scale=0.5]{fig/start_freq}
533 \caption{Selecting the initial frequencies}
541 \begin{algorithmic}[1]
545 \item[$Tcp_i$] array of all computation times for all nodes during one iteration and with highest frequency.
546 \item[$Tcm_i$] array of all communication times for all nodes during one iteration and with highest frequency.
547 \item[$Fmax_i$] array of the maximum frequencies for all nodes.
548 \item[$Pd_i$] array of the dynamic powers for all nodes.
549 \item[$Ps_i$] array of the static powers for all nodes.
550 \item[$Fdiff_i$] array of the difference between two successive frequencies for all nodes.
552 \Ensure $Sopt_1,Sopt_2 \dots, Sopt_N$ is a vector of optimal scaling factors
554 \State $ Scp_i \gets \frac{\max_{i=1,2,\dots,N}(Tcp_i)}{Tcp_i} $
555 \State $F_{i} \gets \frac{Fmax_i}{Scp_i},~{i=1,2,\cdots,N}$
556 \State Round the computed initial frequencies $F_i$ to the closest one available in each node.
557 \If{(not the first frequency)}
558 \State $F_i \gets F_i+Fdiff_i,~i=1,\dots,N.$
560 \State $T_\textit{Old} \gets max_{~i=1,\dots,N } (Tcp_i+Tcm_i)$
561 \State $E_\textit{Original} \gets \sum_{i=1}^{N}{( Pd_i \cdot Tcp_i)} +\sum_{i=1}^{N} {(Ps_i \cdot T_{Old})}$
562 \State $Dist \gets 0$
563 \State $Sopt_{i} \gets 1,~i=1,\dots,N. $
564 \While {(all nodes not reach their minimum frequency)}
565 \If{(not the last freq. \textbf{and} not the slowest node)}
566 \State $F_i \gets F_i - Fdiff_i,~i=1,\dots,N.$
567 \State $S_i \gets \frac{Fmax_i}{F_i},~i=1,\dots,N.$
569 \State $T_{New} \gets max_\textit{~i=1,\dots,N} (Tcp_{i} \cdot S_{i}) + MinTcm $
570 \State $E_\textit{Reduced} \gets \sum_{i=1}^{N}{(S_i^{-2} \cdot Pd_i \cdot Tcp_i)} + $ \hspace*{43 mm}
571 $\sum_{i=1}^{N} {(Ps_i \cdot T_{New})} $
572 \State $ P_\textit{Norm} \gets \frac{T_\textit{Old}}{T_\textit{New}}$
573 \State $E_\textit{Norm}\gets \frac{E_\textit{Reduced}}{E_\textit{Original}}$
574 \If{$(\Pnorm - \Enorm > \Dist)$}
575 \State $Sopt_{i} \gets S_{i},~i=1,\dots,N. $
576 \State $\Dist \gets \Pnorm - \Enorm$
579 \State Return $Sopt_1,Sopt_2,\dots,Sopt_N$
581 \caption{Heterogeneous scaling algorithm}
586 \begin{algorithmic}[1]
588 \For {$k=1$ to \textit{some iterations}}
589 \State Computations section.
590 \State Communications section.
592 \State Gather all times of computation and\newline\hspace*{3em}%
593 communication from each node.
594 \State Call algorithm from Figure~\ref{HSA} with these times.
595 \State Compute the new frequencies from the\newline\hspace*{3em}%
596 returned optimal scaling factors.
597 \State Set the new frequencies to nodes.
601 \caption{DVFS algorithm}
605 \section{Experimental results}
607 To evaluate the efficiency and the overall energy consumption reduction of algorithm~(\ref{HSA}),
608 it was applied to the NAS parallel benchmarks NPB v3.3 \cite{NAS.Parallel.Benchmarks}. The experiments were executed
609 on the simulator SimGrid/SMPI v3.10~\cite{casanova+giersch+legrand+al.2014.versatile} which offers
610 easy tools to create a heterogeneous platform and run message passing applications over it. The
611 heterogeneous platform that was used in the experiments, had one core per node because just one
612 process was executed per node. The heterogeneous platform was composed of four types of nodes.
613 Each type of nodes had different characteristics such as the maximum CPU frequency, the number of
614 available frequencies and the computational power, see table (\ref{table:platform}). The characteristics
615 of these different types of nodes are inspired from the specifications of real Intel processors.
616 The heterogeneous platform had up to 144 nodes and had nodes from the four types in equal proportions,
617 for example if a benchmark was executed on 8 nodes, 2 nodes from each type were used. Since the constructors
618 of CPUs do not specify the dynamic and the static power of their CPUs, for each type of node they were
619 chosen proportionally to its computing power (FLOPS). In the initial heterogeneous platform, while computing
620 with highest frequency, each node consumed power proportional to its computing power which 80\% of it was
621 dynamic power and the rest was 20\% for the static power, the same assumption was made in \cite{Our_first_paper,Rauber_Analytical.Modeling.for.Energy}.
622 Finally, These nodes were connected via an ethernet network with 1 Gbit/s bandwidth.
626 \caption{Heterogeneous nodes characteristics}
629 \begin{tabular}{|*{7}{l|}}
631 Node &Simulated & Max & Min & Diff. & Dynamic & Static \\
632 type &GFLOPS & Freq. & Freq. & Freq. & power & power \\
633 & & GHz & GHz &GHz & & \\
635 1 &40 & 2.5 & 1.2 & 0.1 & 20~w &4~w \\
638 2 &50 & 2.66 & 1.6 & 0.133 & 25~w &5~w \\
641 3 &60 & 2.9 & 1.2 & 0.1 & 30~w &6~w \\
644 4 &70 & 3.4 & 1.6 & 0.133 & 35~w &7~w \\
648 \label{table:platform}
652 %\subsection{Performance prediction verification}
655 \subsection{The experimental results of the scaling algorithm}
659 The proposed algorithm was applied to the seven parallel NAS benchmarks (EP, CG, MG, FT, BT, LU and SP)
660 and the benchmarks were executed with the three classes: A,B and C. However, due to the lack of space in
661 this paper, only the results of the biggest class, C, are presented while being run on different number
662 of nodes, ranging from 4 to 128 or 144 nodes depending on the benchmark being executed. Indeed, the
663 benchmarks CG, MG, LU, EP and FT should be executed on $1, 2, 4, 8, 16, 32, 64, 128$ nodes.
664 The other benchmarks such as BT and SP should be executed on $1, 4, 9, 16, 36, 64, 144$ nodes.
669 \caption{Running NAS benchmarks on 4 nodes }
672 \begin{tabular}{|*{7}{l|}}
674 Method & Execution & Energy & Energy & Performance & Distance \\
675 name & time/s & consumption/J & saving\% & degradation\% & \\
677 CG & 64.64 & 3560.39 &34.16 &6.72 &27.44 \\
679 MG & 18.89 & 1074.87 &35.37 &4.34 &31.03 \\
681 EP &79.73 &5521.04 &26.83 &3.04 &23.79 \\
683 LU &308.65 &21126.00 &34.00 &6.16 &27.84 \\
685 BT &360.12 &21505.55 &35.36 &8.49 &26.87 \\
687 SP &234.24 &13572.16 &35.22 &5.70 &29.52 \\
689 FT &81.58 &4151.48 &35.58 &0.99 &34.59 \\
696 \caption{Running NAS benchmarks on 8 and 9 nodes }
699 \begin{tabular}{|*{7}{l|}}
701 Method & Execution & Energy & Energy & Performance & Distance \\
702 name & time/s & consumption/J & saving\% & degradation\% & \\
704 CG &36.11 &3263.49 &31.25 &7.12 &24.13 \\
706 MG &8.99 &953.39 &33.78 &6.41 &27.37 \\
708 EP &40.39 &5652.81 &27.04 &0.49 &26.55 \\
710 LU &218.79 &36149.77 &28.23 &0.01 &28.22 \\
712 BT &166.89 &23207.42 &32.32 &7.89 &24.43 \\
714 SP &104.73 &18414.62 &24.73 &2.78 &21.95 \\
716 FT &51.10 &4913.26 &31.02 &2.54 &28.48 \\
723 \caption{Running NAS benchmarks on 16 nodes }
726 \begin{tabular}{|*{7}{l|}}
728 Method & Execution & Energy & Energy & Performance & Distance \\
729 name & time/s & consumption/J & saving\% & degradation\% & \\
731 CG &31.74 &4373.90 &26.29 &9.57 &16.72 \\
733 MG &5.71 &1076.19 &32.49 &6.05 &26.44 \\
735 EP &20.11 &5638.49 &26.85 &0.56 &26.29 \\
737 LU &144.13 &42529.06 &28.80 &6.56 &22.24 \\
739 BT &97.29 &22813.86 &34.95 &5.80 &29.15 \\
741 SP &66.49 &20821.67 &22.49 &3.82 &18.67 \\
743 FT &37.01 &5505.60 &31.59 &6.48 &25.11 \\
746 \label{table:res_16n}
750 \caption{Running NAS benchmarks on 32 and 36 nodes }
753 \begin{tabular}{|*{7}{l|}}
755 Method & Execution & Energy & Energy & Performance & Distance \\
756 name & time/s & consumption/J & saving\% & degradation\% & \\
758 CG &32.35 &6704.21 &16.15 &5.30 &10.85 \\
760 MG &4.30 &1355.58 &28.93 &8.85 &20.08 \\
762 EP &9.96 &5519.68 &26.98 &0.02 &26.96 \\
764 LU &99.93 &67463.43 &23.60 &2.45 &21.15 \\
766 BT &48.61 &23796.97 &34.62 &5.83 &28.79 \\
768 SP &46.01 &27007.43 &22.72 &3.45 &19.27 \\
770 FT &28.06 &7142.69 &23.09 &2.90 &20.19 \\
773 \label{table:res_32n}
777 \caption{Running NAS benchmarks on 64 nodes }
780 \begin{tabular}{|*{7}{l|}}
782 Method & Execution & Energy & Energy & Performance & Distance \\
783 name & time/s & consumption/J & saving\% & degradation\% & \\
785 CG &46.65 &17521.83 &8.13 &1.68 &6.45 \\
787 MG &3.27 &1534.70 &29.27 &14.35 &14.92 \\
789 EP &5.05 &5471.1084 &27.12 &3.11 &24.01 \\
791 LU &73.92 &101339.16 &21.96 &3.67 &18.29 \\
793 BT &39.99 &27166.71 &32.02 &12.28 &19.74 \\
795 SP &52.00 &49099.28 &24.84 &0.03 &24.81 \\
797 FT &25.97 &10416.82 &20.15 &4.87 &15.28 \\
800 \label{table:res_64n}
805 \caption{Running NAS benchmarks on 128 and 144 nodes }
808 \begin{tabular}{|*{7}{l|}}
810 Method & Execution & Energy & Energy & Performance & Distance \\
811 name & time/s & consumption/J & saving\% & degradation\% & \\
813 CG &56.92 &41163.36 &4.00 &1.10 &2.90 \\
815 MG &3.55 &2843.33 &18.77 &10.38 &8.39 \\
817 EP &2.67 &5669.66 &27.09 &0.03 &27.06 \\
819 LU &51.23 &144471.90 &16.67 &2.36 &14.31 \\
821 BT &37.96 &44243.82 &23.18 &1.28 &21.90 \\
823 SP &64.53 &115409.71 &26.72 &0.05 &26.67 \\
825 FT &25.51 &18808.72 &12.85 &2.84 &10.01 \\
828 \label{table:res_128n}
830 The overall energy consumption was computed for each instance according to the energy
831 consumption model EQ(\ref{eq:energy}), with and without applying the algorithm. The
832 execution time was also measured for all these experiments. Then, the energy saving
833 and performance degradation percentages were computed for each instance.
834 The results are presented in tables (\ref{table:res_4n}, \ref{table:res_8n}, \ref{table:res_16n},
835 \ref{table:res_32n}, \ref{table:res_64n} and \ref{table:res_128n}). All these results are the
836 average values from many experiments for energy savings and performance degradation.
838 The tables show the experimental results for running the NAS parallel benchmarks on different
839 number of nodes. The experiments show that the algorithm reduce significantly the energy
840 consumption (up to 35\%) and tries to limit the performance degradation. They also show that
841 the energy saving percentage is decreased when the number of the computing nodes is increased.
842 This reduction is due to the increase of the communication times compared to the execution times
843 when the benchmarks are run over a high number of nodes. Indeed, the benchmarks with the same class, C,
844 are executed on different number of nodes, so the computation required for each iteration is divided
845 by the number of computing nodes. On the other hand, more communications are required when increasing
846 the number of nodes so the static energy is increased linearly according to the communication time and
847 the dynamic power is less relevant in the overall energy consumption. Therefore, reducing the frequency
848 with algorithm~(\ref{HSA}) have less effect in reducing the overall energy savings. It can also be
849 noticed that for the benchmarks EP and SP that contain little or no communications, the energy savings
850 are not significantly affected with the high number of nodes. No experiments were conducted using bigger
851 classes such as D, because they require a lot of memory(more than 64GB) when being executed by the simulator
852 on one machine. The maximum distance between the normalized energy curve and the normalized performance
853 for each instance is also shown in the result tables. It is decreased in the same way as the energy
854 saving percentage. The tables also show that the performance degradation percentage is not significantly
855 increased when the number of computing nodes is increased because the computation times are small when
856 compared to the communication times.
862 \subfloat[Energy saving]{%
863 \includegraphics[width=.2315\textwidth]{fig/energy}\label{fig:energy}}%
865 \subfloat[Performance degradation ]{%
866 \includegraphics[width=.2315\textwidth]{fig/per_deg}\label{fig:per_deg}}
868 \caption{The energy and performance for all NAS benchmarks running with difference number of nodes}
871 Plots (\ref{fig:energy} and \ref{fig:per_deg}) present the energy saving and performance degradation
872 respectively for all the benchmarks according to the number of used nodes. As shown in the first plot,
873 the energy saving percentages of the benchmarks MG, LU, BT and FT are decreased linearly when the the
874 number of nodes is increased. While for the EP and SP benchmarks, the energy saving percentage is not
875 affected by the increase of the number of computing nodes, because in these benchmarks there are little or
876 no communications. Finally, the energy saving of the GC benchmark is significantly decreased when the number
877 of nodes is increased because this benchmark has more communications than the others. The second plot
878 shows that the performance degradation percentages of most of the benchmarks are decreased when they
879 run on a big number of nodes because they spend more time communicating than computing, thus, scaling
880 down the frequencies of some nodes have less effect on the performance.
885 \subsection{The results for different power consumption scenarios}
887 The results of the previous section were obtained while using processors that consume during computation
888 an overall power which is 80\% composed of dynamic power and 20\% of static power. In this section,
889 these ratios are changed and two new power scenarios are considered in order to evaluate how the proposed
890 algorithm adapts itself according to the static and dynamic power values. The two new power scenarios
894 \item 70\% dynamic power and 30\% static power
895 \item 90\% dynamic power and 10\% static power
898 The NAS parallel benchmarks were executed again over processors that follow the the new power scenarios.
899 The class C of each benchmark was run over 8 or 9 nodes and the results are presented in tables
900 (\ref{table:res_s1} and \ref{table:res_s2}). These tables show that the energy saving percentage of the 70\%-30\%
901 scenario is less for all benchmarks compared to the energy saving of the 90\%-10\% scenario. Indeed, in the latter
902 more dynamic power is consumed when nodes are running on their maximum frequencies, thus, scaling down the frequency
903 of the nodes results in higher energy savings than in the 70\%-30\% scenario. On the other hand, the performance
904 degradation percentage is less in the 70\%-30\% scenario compared to the 90\%-10\% scenario. This is due to the
905 higher static power percentage in the first scenario which makes it more relevant in the overall consumed energy.
906 Indeed, the static energy is related to the execution time and if the performance is degraded the total consumed
907 static energy is directly increased. Therefore, the proposed algorithm do not scales down much the frequencies of the
908 nodes in order to limit the increase of the execution time and thus limiting the effect of the consumed static energy .
910 The two new power scenarios are compared to the old one in figure (\ref{fig:sen_comp}). It shows the average of
911 the performance degradation, the energy saving and the distances for all NAS benchmarks of class C running on 8 or 9 nodes.
912 The comparison shows that the energy saving ratio is proportional to the dynamic power ratio: it is increased
913 when applying the 90\%-10\% scenario because at maximum frequency the dynamic energy is the the most relevant
914 in the overall consumed energy and can be reduced by lowering the frequency of some processors. On the other hand,
915 the energy saving is decreased when the 70\%-30\% scenario is used because the dynamic energy is less relevant in
916 the overall consumed energy and lowering the frequency do not returns big energy savings.
917 Moreover, the average of the performance degradation is decreased when using a higher ratio for static power
918 (e.g. 70\%-30\% scenario and 80\%-20\% scenario). Since the proposed algorithm optimizes the energy consumption
919 when using a higher ratio for dynamic power the algorithm selects bigger frequency scaling factors that result in
920 more energy saving but less performance, for example see the figure (\ref{fig:scales_comp}). The opposite happens
921 when using a higher ratio for static power, the algorithm proportionally selects smaller scaling values which
922 results in less energy saving but less performance degradation.
926 \caption{The results of 70\%-30\% powers scenario}
929 \begin{tabular}{|*{6}{l|}}
931 Method & Energy & Energy & Performance & Distance \\
932 name & consumption/J & saving\% & degradation\% & \\
934 CG &4144.21 &22.42 &7.72 &14.70 \\
936 MG &1133.23 &24.50 &5.34 &19.16 \\
938 EP &6170.30 &16.19 &0.02 &16.17 \\
940 LU &39477.28 &20.43 &0.07 &20.36 \\
942 BT &26169.55 &25.34 &6.62 &18.71 \\
944 SP &19620.09 &19.32 &3.66 &15.66 \\
946 FT &6094.07 &23.17 &0.36 &22.81 \\
955 \caption{The results of 90\%-10\% powers scenario}
958 \begin{tabular}{|*{6}{l|}}
960 Method & Energy & Energy & Performance & Distance \\
961 name & consumption/J & saving\% & degradation\% & \\
963 CG &2812.38 &36.36 &6.80 &29.56 \\
965 MG &825.427 &38.35 &6.41 &31.94 \\
967 EP &5281.62 &35.02 &2.68 &32.34 \\
969 LU &31611.28 &39.15 &3.51 &35.64 \\
971 BT &21296.46 &36.70 &6.60 &30.10 \\
973 SP &15183.42 &35.19 &11.76 &23.43 \\
975 FT &3856.54 &40.80 &5.67 &35.13 \\
984 \subfloat[Comparison the average of the results on 8 nodes]{%
985 \includegraphics[width=.22\textwidth]{fig/sen_comp}\label{fig:sen_comp}}%
987 \subfloat[Comparison the selected frequency scaling factors of MG benchmark class C running on 8 nodes]{%
988 \includegraphics[width=.24\textwidth]{fig/three_scenarios}\label{fig:scales_comp}}
990 \caption{The comparison of the three power scenarios}
995 \subsection{The verifications of the proposed method}
997 The precision of the proposed algorithm mainly depends on the execution time prediction model defined in
998 EQ(\ref{eq:perf}) and the energy model computed by EQ(\ref{eq:energy}).
999 The energy model is also significantly dependent on the execution time model because the static energy is
1000 linearly related the execution time and the dynamic energy is related to the computation time. So, all of
1001 the work presented in this paper is based on the execution time model. To verify this model, the predicted
1002 execution time was compared to the real execution time over Simgrid for all the NAS parallel benchmarks
1003 running class B on 8 or 9 nodes. The comparison showed that the proposed execution time model is very precise,
1004 the maximum normalized difference between the predicted execution time and the real execution time is equal
1005 to 0.03 for all the NAS benchmarks.
1007 Since the proposed algorithm is not an exact method and do not test all the possible solutions (vectors of scaling factors)
1008 in the search space and to prove its efficiency, it was compared on small instances to a brute force search algorithm
1009 that tests all the possible solutions. The brute force algorithm was applied to different NAS benchmarks classes with
1010 different number of nodes. The solutions returned by the brute force algorithm and the proposed algorithm were identical
1011 and the proposed algorithm was on average 10 times faster than the brute force algorithm. It has a small execution time:
1012 for a heterogeneous cluster composed of four different types of nodes having the characteristics presented in
1013 table~(\ref{table:platform}), it takes on average \np[ms]{0.04} for 4 nodes and \np[ms]{0.15} on average for 144 nodes
1014 to compute the best scaling factors vector. The algorithm complexity is $O(F\cdot (N \cdot4) )$, where $F$ is the number
1015 of iterations and $N$ is the number of computing nodes. The algorithm needs from 12 to 20 iterations to select the best
1016 vector of frequency scaling factors that gives the results of the sections (\ref{sec.res}) and (\ref{sec.compare}) .
1018 \section{Conclusion}
1020 In this paper, we have presented a new online heterogeneous scaling algorithm
1021 that selects the best possible vector of frequency scaling factors. This vector
1022 gives the maximum distance (optimal tradeoff) between the normalized energy and
1023 the performance curves. In addition, we developed a new energy model for measuring
1024 and predicting the energy of distributed iterative applications running over heterogeneous
1025 cluster. The proposed method evaluated on Simgrid/SMPI simulator to built a heterogeneous
1026 platform to executes NAS parallel benchmarks. The results of the experiments showed the ability of
1027 the proposed algorithm to changes its behaviour to selects different scaling factors when
1028 the number of computing nodes and both of the static and the dynamic powers are changed.
1030 In the future, we plan to improve this method to apply on asynchronous iterative applications
1031 where each task does not wait the others tasks to finish there works. This leads us to develop a new
1032 energy model to an asynchronous iterative applications, where the number of iterations is not
1033 known in advance and depends on the global convergence of the iterative system.
1035 \section*{Acknowledgment}
1039 % trigger a \newpage just before the given reference
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1045 \bibliographystyle{IEEEtran}
1046 \bibliography{IEEEabrv,my_reference}
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1056 % LocalWords: Fanfakh Charr FIXME Tianhe DVFS HPC NAS NPB SMPI Rauber's Rauber
1057 % LocalWords: CMOS EQ EPSA Franche Comté Tflop Rünger IUT Maréchal Juin cedex
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1059 % LocalWords: Scp Fmax Fdiff SimGrid GFlops Xeon EP BT