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62 \title{Energy Consumption Reduction for Message Passing Iterative Applications in Heterogeneous Architecture Using DVFS}
72 FEMTO-ST Institute, University of Franche-Comte\\
73 IUT de Belfort-Montbéliard,
74 19 avenue du Maréchal Juin, BP 527, 90016 Belfort cedex, France\\
75 % Telephone: \mbox{+33 3 84 58 77 86}, % Raphaël
76 % Fax: \mbox{+33 3 84 58 77 81}\\ % Dept Info
77 Email: \email{{jean-claude.charr,raphael.couturier,ahmed.fanfakh_badri_muslim,arnaud.giersch}@univ-fcomte.fr}
84 Computing platforms are consuming more and more energy due to the increasing
85 number of nodes composing them. To minimize the operating costs of these
86 platforms many techniques have been used. Dynamic voltage and frequency scaling
87 (DVFS) is one of them. It reduces the frequency of a CPU to lower its energy
88 consumption. However, lowering the frequency of a CPU might increase the
89 execution time of an application running on that processor. Therefore, the
90 frequency that gives the best trade-off between the energy consumption and the
91 performance of an application must be selected.\\
92 In this paper, a new online frequencies selecting algorithm for heterogeneous
93 platforms is presented. It selects the frequency which tries to give the best
94 trade-off between energy saving and performance degradation, for each node
95 computing the message passing iterative application. The algorithm has a small
96 overhead and works without training or profiling. It uses a new energy model for
97 message passing iterative applications running on a heterogeneous platform. The
98 proposed algorithm is evaluated on the SimGrid simulator while running the NAS
99 parallel benchmarks. The experiments show that it reduces the energy
100 consumption by up to 35\% while limiting the performance degradation as much as
101 possible. Finally, the algorithm is compared to an existing method, the
102 comparison results showing that it outperforms the latter.
106 \section{Introduction}
108 The need for more computing power is continually increasing. To partially
109 satisfy this need, most supercomputers constructors just put more computing
110 nodes in their platform. The resulting platforms might achieve higher floating
111 point operations per second (FLOPS), but the energy consumption and the heat
112 dissipation are also increased. As an example, the Chinese supercomputer
113 Tianhe-2 had the highest FLOPS in November 2014 according to the Top500 list
114 \cite{TOP500_Supercomputers_Sites}. However, it was also the most power hungry
115 platform with its over 3 million cores consuming around 17.8 megawatts.
116 Moreover, according to the U.S. annual energy outlook 2014
117 \cite{U.S_Annual.Energy.Outlook.2014}, the price of energy for 1 megawatt-hour
118 was approximately equal to \$70. Therefore, the price of the energy consumed by
119 the Tianhe-2 platform is approximately more than \$10 million each year. The
120 computing platforms must be more energy efficient and offer the highest number
121 of FLOPS per watt possible, such as the L-CSC from the GSI Helmholtz Center
122 which became the top of the Green500 list in November 2014 \cite{Green500_List}.
123 This heterogeneous platform executes more than 5 GFLOPS per watt while consuming
126 Besides platform improvements, there are many software and hardware techniques
127 to lower the energy consumption of these platforms, such as scheduling, DVFS,
128 \dots{} DVFS is a widely used process to reduce the energy consumption of a
129 processor by lowering its frequency
130 \cite{Rizvandi_Some.Observations.on.Optimal.Frequency}. However, it also reduces
131 the number of FLOPS executed by the processor which might increase the execution
132 time of the application running over that processor. Therefore, researchers use
133 different optimization strategies to select the frequency that gives the best
134 trade-off between the energy reduction and performance degradation ratio. In
135 \cite{Our_first_paper}, a frequency selecting algorithm was proposed to reduce
136 the energy consumption of message passing iterative applications running over
137 homogeneous platforms. The results of the experiments show significant energy
138 consumption reductions. In this paper, a new frequency selecting algorithm
139 adapted for heterogeneous platform is presented. It selects the vector of
140 frequencies, for a heterogeneous platform running a message passing iterative
141 application, that simultaneously tries to offer the maximum energy reduction and
142 minimum performance degradation ratio. The algorithm has a very small overhead,
143 works online and does not need any training or profiling.
145 This paper is organized as follows: Section~\ref{sec.relwork} presents some
146 related works from other authors. Section~\ref{sec.exe} describes how the
147 execution time of message passing programs can be predicted. It also presents an energy
148 model that predicts the energy consumption of an application running over a heterogeneous platform. Section~\ref{sec.compet} presents
149 the energy-performance objective function that maximizes the reduction of energy
150 consumption while minimizing the degradation of the program's performance.
151 Section~\ref{sec.optim} details the proposed frequency selecting algorithm then the precision of the proposed algorithm is verified.
152 Section~\ref{sec.expe} presents the results of applying the algorithm on the NAS parallel benchmarks and executing them
153 on a heterogeneous platform. It shows the results of running three
154 different power scenarios and comparing them. Moreover, it also shows the comparison results
155 between the proposed method and an existing method.
156 Finally, in Section~\ref{sec.concl} the paper ends with a summary and some future works.
158 \section{Related works}
160 DVFS is a technique used in modern processors to scale down both the voltage and
161 the frequency of the CPU while computing, in order to reduce the energy
162 consumption of the processor. DVFS is also allowed in GPUs to achieve the same
163 goal. Reducing the frequency of a processor lowers its number of FLOPS and might
164 degrade the performance of the application running on that processor, especially
165 if it is compute bound. Therefore selecting the appropriate frequency for a
166 processor to satisfy some objectives while taking into account all the
167 constraints, is not a trivial operation. Many researchers used different
168 strategies to tackle this problem. Some of them developed online methods that
169 compute the new frequency while executing the application, such
170 as~\cite{Hao_Learning.based.DVFS,Spiliopoulos_Green.governors.Adaptive.DVFS}.
171 Others used offline methods that might need to run the application and profile
172 it before selecting the new frequency, such
173 as~\cite{Rountree_Bounding.energy.consumption.in.MPI,Cochran_Pack_and_Cap_Adaptive_DVFS}.
174 The methods could be heuristics, exact or brute force methods that satisfy
175 varied objectives such as energy reduction or performance. They also could be
176 adapted to the execution's environment and the type of the application such as
177 sequential, parallel or distributed architecture, homogeneous or heterogeneous
178 platform, synchronous or asynchronous application, \dots{}
180 In this paper, we are interested in reducing energy for message passing iterative synchronous applications running over heterogeneous platforms.
181 Some works have already been done for such platforms and they can be classified into two types of heterogeneous platforms:
184 \item the platform is composed of homogeneous GPUs and homogeneous CPUs.
185 \item the platform is only composed of heterogeneous CPUs.
189 For the first type of platform, the computing intensive parallel tasks are
190 executed on the GPUs and the rest are executed on the CPUs. Luley et
191 al.~\cite{Luley_Energy.efficiency.evaluation.and.benchmarking}, proposed a
192 heterogeneous cluster composed of Intel Xeon CPUs and NVIDIA GPUs. Their main
193 goal was to maximize the energy efficiency of the platform during computation by
194 maximizing the number of FLOPS per watt generated.
195 In~\cite{KaiMa_Holistic.Approach.to.Energy.Efficiency.in.GPU-CPU}, Kai Ma et
196 al. developed a scheduling algorithm that distributes workloads proportional to
197 the computing power of the nodes which could be a GPU or a CPU. All the tasks
198 must be completed at the same time. In~\cite{Rong_Effects.of.DVFS.on.K20.GPU},
199 Rong et al. showed that a heterogeneous (GPUs and CPUs) cluster that enables
200 DVFS gave better energy and performance efficiency than other clusters only
203 The work presented in this paper concerns the second type of platform, with
204 heterogeneous CPUs. Many methods were conceived to reduce the energy
205 consumption of this type of platform. Naveen et
206 al.~\cite{Naveen_Power.Efficient.Resource.Scaling} developed a method that
207 minimizes the value of $\mathit{energy}\times \mathit{delay}^2$ (the delay is
208 the sum of slack times that happen during synchronous communications) by
209 dynamically assigning new frequencies to the CPUs of the heterogeneous
210 cluster. Lizhe et al.~\cite{Lizhe_Energy.aware.parallel.task.scheduling}
211 proposed an algorithm that divides the executed tasks into two types: the
212 critical and non critical tasks. The algorithm scales down the frequency of non
213 critical tasks proportionally to their slack and communication times while
214 limiting the performance degradation percentage to less than
215 10\%. In~\cite{Joshi_Blackbox.prediction.of.impact.of.DVFS}, they developed a
216 heterogeneous cluster composed of two types of Intel and AMD processors. They
217 use a gradient method to predict the impact of DVFS operations on performance.
218 In~\cite{Shelepov_Scheduling.on.Heterogeneous.Multicore} and
219 \cite{Li_Minimizing.Energy.Consumption.for.Frame.Based.Tasks}, the best
220 frequencies for a specified heterogeneous cluster are selected offline using
221 some heuristic. Chen et
222 al.~\cite{Chen_DVFS.under.quality.of.service.requirements} used a greedy dynamic
223 programming approach to minimize the power consumption of heterogeneous servers
224 while respecting given time constraints. This approach had considerable
225 overhead. In contrast to the above described papers, this paper presents the
226 following contributions :
228 \item two new energy and performance models for message passing iterative synchronous applications running over
229 a heterogeneous platform. Both models take into account communication and slack times. The models can predict the required energy and the execution time of the application.
231 \item a new online frequency selecting algorithm for heterogeneous platforms. The algorithm has a very small
232 overhead and does not need 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.
236 \section{The performance and energy consumption measurements on heterogeneous architecture}
241 \subsection{The execution time of message passing distributed
242 iterative applications on a heterogeneous platform}
244 In this paper, we are interested in reducing the energy consumption of message
245 passing distributed iterative synchronous applications running over
246 heterogeneous platforms. A heterogeneous platform is defined as a collection of
247 heterogeneous computing nodes interconnected via a high speed homogeneous
248 network. Therefore, each node has different characteristics such as computing
249 power (FLOPS), energy consumption, CPU's frequency range, \dots{} but they all
250 have the same network bandwidth and latency.
252 The overall execution time of a distributed iterative synchronous application
253 over a heterogeneous platform consists of the sum of the computation time and
254 the communication time for every iteration on a node. However, due to the
255 heterogeneous computation power of the computing nodes, slack times might occur
256 when fast nodes have to wait, during synchronous communications, for the slower
257 nodes to finish their computations (see Figure~\ref{fig:heter}). Therefore, the
258 overall execution time of the program is the execution time of the slowest task
259 which has the highest computation time and no slack time.
263 \includegraphics[scale=0.6]{fig/commtasks}
264 \caption{Parallel tasks on a heterogeneous platform}
268 Dynamic Voltage and Frequency Scaling (DVFS) is a process, implemented in
269 modern processors, that reduces the energy consumption of a CPU by scaling
270 down its voltage and frequency. Since DVFS lowers the frequency of a CPU
271 and consequently its computing power, the execution time of a program running
272 over that scaled down processor might increase, especially if the program is
273 compute bound. The frequency reduction process can be expressed by the scaling
274 factor S which is the ratio between the maximum and the new frequency of a CPU
278 S = \frac{\Fmax}{\Fnew}
280 The execution time of a compute bound sequential program is linearly proportional
281 to the frequency scaling factor $S$. On the other hand, message passing
282 distributed applications consist of two parts: computation and communication.
283 The execution time of the computation part is linearly proportional to the
284 frequency scaling factor $S$ but the communication time is not affected by the
285 scaling factor because the processors involved remain idle during the
286 communications~\cite{Freeh_Exploring.the.Energy.Time.Tradeoff}.
287 The communication time for a task is the summation of periods of
288 time that begin with an MPI call for sending or receiving a message
289 until the message is synchronously sent or received.
291 Since in a heterogeneous platform each node has different characteristics,
292 especially different frequency gears, when applying DVFS operations on these
293 nodes, they may get different scaling factors represented by a scaling vector:
294 $(S_1, S_2,\dots, S_N)$ where $S_i$ is the scaling factor of processor $i$. To
295 be able to predict the execution time of message passing synchronous iterative
296 applications running over a heterogeneous platform, for different vectors of
297 scaling factors, the communication time and the computation time for all the
298 tasks must be measured during the first iteration before applying any DVFS
299 operation. Then the execution time for one iteration of the application with any
300 vector of scaling factors can be predicted using (\ref{eq:perf}).
303 \Tnew = \max_{i=1,2,\dots,N} ({\TcpOld[i]} \cdot S_{i}) + \MinTcm
308 \MinTcm = \min_{i=1,2,\dots,N} (\Tcm[i])
310 where $\TcpOld[i]$ is the computation time of processor $i$ during the first
311 iteration and $\MinTcm$ is the communication time of the slowest processor from
312 the first iteration. The model computes the maximum computation time with
313 scaling factor from each node added to the communication time of the slowest
314 node. It means only the communication time without any slack time is taken into
315 account. Therefore, the execution time of the iterative application is equal to
316 the execution time of one iteration as in (\ref{eq:perf}) multiplied by the
317 number of iterations of that application.
319 This prediction model is developed from the model to predict the execution time
320 of message passing distributed applications for homogeneous
321 architectures~\cite{Our_first_paper}. The execution time prediction model is
322 used in the method to optimize both the energy consumption and the performance of
323 iterative methods, which is presented in the following sections.
326 \subsection{Energy model for heterogeneous platform}
327 Many researchers~\cite{Malkowski_energy.efficient.high.performance.computing,
328 Rauber_Analytical.Modeling.for.Energy,Zhuo_Energy.efficient.Dynamic.Task.Scheduling,
329 Rizvandi_Some.Observations.on.Optimal.Frequency} divide the power consumed by a processor into
330 two power metrics: the static and the dynamic power. While the first one is
331 consumed as long as the computing unit is turned on, the latter is only consumed during
332 computation times. The dynamic power $\Pd$ is related to the switching
333 activity $\alpha$, load capacitance $\CL$, the supply voltage $V$ and
334 operational frequency $F$, as shown in (\ref{eq:pd}).
337 \Pd = \alpha \cdot \CL \cdot V^2 \cdot F
339 The static power $\Ps$ captures the leakage power as follows:
342 \Ps = V \cdot \Ntrans \cdot \Kdesign \cdot \Ileak
344 where V is the supply voltage, $\Ntrans$ is the number of transistors,
345 $\Kdesign$ is a design dependent parameter and $\Ileak$ is a
346 technology dependent parameter. The energy consumed by an individual processor
347 to execute a given program can be computed as:
350 \Eind = \Pd \cdot \Tcp + \Ps \cdot T
352 where $T$ is the execution time of the program, $\Tcp$ is the computation
353 time and $\Tcp \le T$. $\Tcp$ may be equal to $T$ if there is no
354 communication and no slack time.
356 The main objective of DVFS operation is to reduce the overall energy consumption~\cite{Le_DVFS.Laws.of.Diminishing.Returns}.
357 The operational frequency $F$ depends linearly on the supply voltage $V$, i.e., $V = \beta \cdot F$ with some
358 constant $\beta$.~This equation is used to study the change of the dynamic
359 voltage with respect to various frequency values in~\cite{Rauber_Analytical.Modeling.for.Energy}. The reduction
360 process of the frequency can be expressed by the scaling factor $S$ which is the
361 ratio between the maximum and the new frequency as in (\ref{eq:s}).
362 The CPU governors are power schemes supplied by the operating
363 system's kernel to lower a core's frequency. The new frequency
364 $\Fnew$ from (\ref{eq:s}) can be calculated as follows:
367 \Fnew = S^{-1} \cdot \Fmax
369 Replacing $\Fnew$ in (\ref{eq:pd}) as in (\ref{eq:fnew}) gives the following
370 equation for dynamic power consumption:
373 \PdNew = \alpha \cdot \CL \cdot V^2 \cdot \Fnew = \alpha \cdot \CL \cdot \beta^2 \cdot \Fnew^3 \\
374 {} = \alpha \cdot \CL \cdot V^2 \cdot \Fmax \cdot S^{-3} = \PdOld \cdot S^{-3}
376 where $\PdNew$ and $\PdOld$ are the dynamic power consumed with the
377 new frequency and the maximum frequency respectively.
379 According to (\ref{eq:pdnew}) the dynamic power is reduced by a factor of $S^{-3}$ when
380 reducing the frequency by a factor of $S$~\cite{Rauber_Analytical.Modeling.for.Energy}. Since the FLOPS of a CPU is proportional
381 to the frequency of a CPU, the computation time is increased proportionally to $S$.
382 The new dynamic energy is the dynamic power multiplied by the new time of computation
383 and is given by the following equation:
386 \EdNew = \PdOld \cdot S^{-3} \cdot (\Tcp \cdot S)= S^{-2}\cdot \PdOld \cdot \Tcp
388 The static power is related to the power leakage of the CPU and is consumed during computation
389 and even when idle. As in~\cite{Rauber_Analytical.Modeling.for.Energy,Zhuo_Energy.efficient.Dynamic.Task.Scheduling},
390 the static power of a processor is considered as constant
391 during idle and computation periods, and for all its available frequencies.
392 The static energy is the static power multiplied by the execution time of the program.
393 According to the execution time model in (\ref{eq:perf}), the execution time of the program
394 is the sum of the computation and the communication times. The computation time is linearly related
395 to the frequency scaling factor, while this scaling factor does not affect the communication time.
396 The static energy of a processor after scaling its frequency is computed as follows:
399 \Es = \Ps \cdot (\Tcp \cdot S + \Tcm)
402 In the considered heterogeneous platform, each processor $i$ might have
403 different dynamic and static powers, noted as $\Pd[i]$ and $\Ps[i]$
404 respectively. Therefore, even if the distributed message passing iterative
405 application is load balanced, the computation time of each CPU $i$ noted
406 $\Tcp[i]$ might be different and different frequency scaling factors might be
407 computed in order to decrease the overall energy consumption of the application
408 and reduce slack times. The communication time of a processor $i$ is noted as
409 $\Tcm[i]$ and could contain slack times when communicating with slower
410 nodes, see Figure~\ref{fig:heter}. Therefore, all nodes do not have equal
411 communication times. While the dynamic energy is computed according to the
412 frequency scaling factor and the dynamic power of each node as in
413 (\ref{eq:Edyn}), the static energy is computed as the sum of the execution time
414 of one iteration multiplied by the static power of each processor. The overall
415 energy consumption of a message passing distributed application executed over a
416 heterogeneous platform during one iteration is the summation of all dynamic and
417 static energies for each processor. It is computed as follows:
420 E = \sum_{i=1}^{N} {(S_i^{-2} \cdot \Pd[i] \cdot \Tcp[i])} + {} \\
421 \sum_{i=1}^{N} (\Ps[i] \cdot (\max_{i=1,2,\dots,N} (\Tcp[i] \cdot S_{i}) +
425 Reducing the frequencies of the processors according to the vector of
426 scaling factors $(S_1, S_2,\dots, S_N)$ may degrade the performance of the
427 application and thus, increase the static energy because the execution time is
428 increased~\cite{Kim_Leakage.Current.Moore.Law}. The overall energy consumption for the iterative
429 application can be measured by measuring the energy consumption for one iteration as in (\ref{eq:energy})
430 multiplied by the number of iterations of that application.
433 \section{Optimization of both energy consumption and performance}
436 Using the lowest frequency for each processor does not necessarily give the most
437 energy efficient execution of an application. Indeed, even though the dynamic
438 power is reduced while scaling down the frequency of a processor, its
439 computation power is proportionally decreased. Hence, the execution time might
440 be drastically increased and during that time, dynamic and static powers are
441 being consumed. Therefore, it might cancel any gains achieved by scaling down
442 the frequency of all nodes to the minimum and the overall energy consumption of
443 the application might not be the optimal one. It is not trivial to select the
444 appropriate frequency scaling factor for each processor while considering the
445 characteristics of each processor (computation power, range of frequencies,
446 dynamic and static powers) and the task executed (computation/communication
447 ratio). The aim being to reduce the overall energy consumption and to avoid
448 increasing significantly the execution time. In our previous
449 work~\cite{Our_first_paper}, we proposed a method that selects the optimal
450 frequency scaling factor for a homogeneous cluster executing a message passing
451 iterative synchronous application while giving the best trade-off between the
452 energy consumption and the performance for such applications. In this work we
453 are interested in heterogeneous clusters as described above. Due to the
454 heterogeneity of the processors, a vector of scaling factors should
455 be selected and it must give the best trade-off between energy consumption and
458 The relation between the energy consumption and the execution time for an
459 application is complex and nonlinear, Thus, unlike the relation between the
460 execution time and the scaling factor, the relation between the energy and the
461 frequency scaling factors is nonlinear, for more details refer
462 to~\cite{Freeh_Exploring.the.Energy.Time.Tradeoff}. Moreover, these relations
463 are not measured using the same metric. To solve this problem, the execution
464 time is normalized by computing the ratio between the new execution time (after
465 scaling down the frequencies of some processors) and the initial one (with
466 maximum frequency for all nodes) as follows:
469 \Pnorm = \frac{\Tnew}{\Told}\\
470 {} = \frac{ \max_{i=1,2,\dots,N} (\Tcp[i] \cdot S_{i}) +\MinTcm}
471 {\max_{i=1,2,\dots,N}{(\Tcp[i]+\Tcm[i])}}
475 In the same way, the energy is normalized by computing the ratio between the consumed energy
476 while scaling down the frequency and the consumed energy with maximum frequency for all nodes:
479 \Enorm = \frac{\Ereduced}{\Eoriginal} \\
480 {} = \frac{ \sum_{i=1}^{N}{(S_i^{-2} \cdot \Pd[i] \cdot \Tcp[i])} +
481 \sum_{i=1}^{N} {(\Ps[i] \cdot \Tnew)}}{\sum_{i=1}^{N}{( \Pd[i] \cdot \Tcp[i])} +
482 \sum_{i=1}^{N} {(\Ps[i] \cdot \Told)}}
484 Where $\Ereduced$ and $\Eoriginal$ are computed using (\ref{eq:energy}) and
485 $\Tnew$ and $\Told$ are computed as in (\ref{eq:pnorm}).
488 goal is to optimize the energy and execution time at the same time, the normalized
489 energy and execution time curves are not in the same direction. According
490 to the equations~(\ref{eq:pnorm}) and (\ref{eq:enorm}), the vector of frequency
491 scaling factors $S_1,S_2,\dots,S_N$ reduce both the energy and the execution
492 time simultaneously. But the main objective is to produce maximum energy
493 reduction with minimum execution time reduction.
495 This problem can be solved by making the optimization process for energy and
496 execution time following the same direction. Therefore, the equation of the
497 normalized execution time is inverted which gives the normalized performance equation, as follows:
500 \Pnorm = \frac{\Told}{\Tnew}\\
501 = \frac{\max_{i=1,2,\dots,N}{(\Tcp[i]+\Tcm[i])}}
502 { \max_{i=1,2,\dots,N} (\Tcp[i] \cdot S_{i}) + \MinTcm}
508 \subfloat[Homogeneous platform]{%
509 \includegraphics[width=.33\textwidth]{fig/homo}\label{fig:r1}}%
512 \subfloat[Heterogeneous platform]{%
513 \includegraphics[width=.33\textwidth]{fig/heter}\label{fig:r2}}
515 \caption{The energy and performance relation}
518 Then, the objective function can be modeled in order to find the maximum
519 distance between the energy curve (\ref{eq:enorm}) and the performance curve
520 (\ref{eq:pnorm_inv}) over all available sets of scaling factors. This
521 represents the minimum energy consumption with minimum execution time (maximum
522 performance) at the same time, see Figure~\ref{fig:r1} or
523 Figure~\ref{fig:r2}. Then the objective function has the following form:
527 \mathop{\max_{i=1,\dots F}}_{j=1,\dots,N}
528 (\overbrace{\Pnorm(S_{ij})}^{\text{Maximize}} -
529 \overbrace{\Enorm(S_{ij})}^{\text{Minimize}} )
531 where $N$ is the number of nodes and $F$ is the number of available frequencies for each node.
532 Then, the optimal set of scaling factors that satisfies (\ref{eq:max}) can be selected.
533 The objective function can work with any energy model or any power values for each node
534 (static and dynamic powers). However, the most important energy reduction gain can be achieved when
535 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}.
537 \section{The scaling factors selection algorithm for heterogeneous platforms }
540 \subsection{The algorithm details}
541 In this section, Algorithm~\ref{HSA} is presented. It selects the frequency
542 scaling factors vector that gives the best trade-off between minimizing the
543 energy consumption and maximizing the performance of a message passing
544 synchronous iterative application executed on a heterogeneous platform. It works
545 online during the execution time of the iterative message passing program. It
546 uses information gathered during the first iteration such as the computation
547 time and the communication time in one iteration for each node. The algorithm is
548 executed after the first iteration and returns a vector of optimal frequency
549 scaling factors that satisfies the objective function (\ref{eq:max}). The
550 program applies DVFS operations to change the frequencies of the CPUs according
551 to the computed scaling factors. This algorithm is called just once during the
552 execution of the program. Algorithm~\ref{dvfs} shows where and when the proposed
553 scaling algorithm is called in the iterative MPI program.
555 The nodes in a heterogeneous platform have different computing powers, thus
556 while executing message passing iterative synchronous applications, fast nodes
557 have to wait for the slower ones to finish their computations before being able
558 to synchronously communicate with them as in Figure~\ref{fig:heter}. These
559 periods are called idle or slack times. The algorithm takes into account this
560 problem and tries to reduce these slack times when selecting the frequency
561 scaling factors vector. At first, it selects initial frequency scaling factors
562 that increase the execution times of fast nodes and minimize the differences
563 between the computation times of fast and slow nodes. The value of the initial
564 frequency scaling factor for each node is inversely proportional to its
565 computation time that was gathered from the first iteration. These initial
566 frequency scaling factors are computed as a ratio between the computation time
567 of the slowest node and the computation time of the node $i$ as follows:
570 \Scp[i] = \frac{\max_{i=1,2,\dots,N}(\Tcp[i])}{\Tcp[i]}
572 Using the initial frequency scaling factors computed in (\ref{eq:Scp}), the algorithm computes
573 the initial frequencies for all nodes as a ratio between the maximum frequency of node $i$
574 and the computation scaling factor $\Scp[i]$ as follows:
577 F_{i} = \frac{\Fmax[i]}{\Scp[i]},~{i=1,2,\dots,N}
579 If the computed initial frequency for a node is not available in the gears of
580 that node, it is replaced by the nearest available frequency. In
581 Figure~\ref{fig:st_freq}, the nodes are sorted by their computing power in
582 ascending order and the frequencies of the faster nodes are scaled down
583 according to the computed initial frequency scaling factors. The resulting new
584 frequencies are colored in blue in Figure~\ref{fig:st_freq}. This set of
585 frequencies can be considered as a higher bound for the search space of the
586 optimal vector of frequencies because selecting frequency scaling factors higher
587 than the higher bound will not improve the performance of the application and it
588 will increase its overall energy consumption. Therefore the algorithm that
589 selects the frequency scaling factors starts the search method from these
590 initial frequencies and takes a downward search direction toward lower
591 frequencies. The algorithm iterates on all left frequencies, from the higher
592 bound until all nodes reach their minimum frequencies, to compute their overall
593 energy consumption and performance, and select the optimal frequency scaling
594 factors vector. At each iteration the algorithm determines the slowest node
595 according to the equation (\ref{eq:perf}) and keeps its frequency unchanged,
596 while it lowers the frequency of all other nodes by one gear. The new overall
597 energy consumption and execution time are computed according to the new scaling
598 factors. The optimal set of frequency scaling factors is the set that gives the
599 highest distance according to the objective function (\ref{eq:max}).
601 Figures~\ref{fig:r1} and \ref{fig:r2} illustrate the normalized performance and
602 consumed energy for an application running on a homogeneous platform and a
603 heterogeneous platform respectively while increasing the scaling factors. It can
604 be noticed that in a homogeneous platform the search for the optimal scaling
605 factor should start from the maximum frequency because the performance and the
606 consumed energy decrease from the beginning of the plot. On the other hand,
607 in the heterogeneous platform the performance is maintained at the beginning of
608 the plot even if the frequencies of the faster nodes decrease until the
609 computing power of scaled down nodes are lower than the slowest node. In other
610 words, until they reach the higher bound. It can also be noticed that the higher
611 the difference between the faster nodes and the slower nodes is, the bigger the
612 maximum distance between the energy curve and the performance curve is while
613 the scaling factors are varying which results in bigger energy savings.
616 \includegraphics[scale=0.5]{fig/start_freq}
617 \caption{Selecting the initial frequencies}
625 \begin{algorithmic}[1]
629 \item[{$\Tcp[i]$}] array of all computation times for all nodes during one iteration and with highest frequency.
630 \item[{$\Tcm[i]$}] array of all communication times for all nodes during one iteration and with highest frequency.
631 \item[{$\Fmax[i]$}] array of the maximum frequencies for all nodes.
632 \item[{$\Pd[i]$}] array of the dynamic powers for all nodes.
633 \item[{$\Ps[i]$}] array of the static powers for all nodes.
634 \item[{$\Fdiff[i]$}] array of the difference between two successive frequencies for all nodes.
636 \Ensure $\Sopt[1],\Sopt[2] \dots, \Sopt[N]$ is a vector of optimal scaling factors
638 \State $\Scp[i] \gets \frac{\max_{i=1,2,\dots,N}(\Tcp[i])}{\Tcp[i]} $
639 \State $F_{i} \gets \frac{\Fmax[i]}{\Scp[i]},~{i=1,2,\cdots,N}$
640 \State Round the computed initial frequencies $F_i$ to the closest one available in each node.
641 \If{(not the first frequency)}
642 \State $F_i \gets F_i+\Fdiff[i],~i=1,\dots,N.$
644 \State $\Told \gets \max_{i=1,\dots,N} (\Tcp[i]+\Tcm[i])$
645 % \State $\Eoriginal \gets \sum_{i=1}^{N}{( \Pd[i] \cdot \Tcp[i])} +\sum_{i=1}^{N} {(\Ps[i] \cdot \Told)}$
646 \State $\Eoriginal \gets \sum_{i=1}^{N}{( \Pd[i] \cdot \Tcp[i] + \Ps[i] \cdot \Told)}$
647 \State $\Sopt[i] \gets 1,~i=1,\dots,N. $
648 \State $\Dist \gets 0 $
649 \While {(all nodes not reach their minimum frequency)}
650 \If{(not the last freq. \textbf{and} not the slowest node)}
651 \State $F_i \gets F_i - \Fdiff[i],~i=1,\dots,N.$
652 \State $S_i \gets \frac{\Fmax[i]}{F_i},~i=1,\dots,N.$
654 \State $\Tnew \gets \max_{i=1,\dots,N} (\Tcp[i] \cdot S_{i}) + \MinTcm $
655 % \State $\Ereduced \gets \sum_{i=1}^{N}{(S_i^{-2} \cdot \Pd[i] \cdot \Tcp[i])} + \sum_{i=1}^{N} {(\Ps[i] \cdot \rlap{\Tnew)}} $
656 \State $\Ereduced \gets \sum_{i=1}^{N}{(S_i^{-2} \cdot \Pd[i] \cdot \Tcp[i] + \Ps[i] \cdot \rlap{\Tnew)}} $
657 \State $\Pnorm \gets \frac{\Told}{\Tnew}$
658 \State $\Enorm\gets \frac{\Ereduced}{\Eoriginal}$
659 \If{$(\Pnorm - \Enorm > \Dist)$}
660 \State $\Sopt[i] \gets S_{i},~i=1,\dots,N. $
661 \State $\Dist \gets \Pnorm - \Enorm$
664 \State Return $\Sopt[1],\Sopt[2],\dots,\Sopt[N]$
666 \caption{frequency scaling factors selection algorithm}
671 \begin{algorithmic}[1]
673 \For {$k=1$ to \textit{some iterations}}
674 \State Computations section.
675 \State Communications section.
677 \State Gather all times of computation and\newline\hspace*{3em}%
678 communication from each node.
679 \State Call Algorithm \ref{HSA}.
680 \State Compute the new frequencies from the\newline\hspace*{3em}%
681 returned optimal scaling factors.
682 \State Set the new frequencies to nodes.
686 \caption{DVFS algorithm}
690 \subsection{The evaluation of the proposed algorithm}
691 \label{sec.verif.algo}
692 The precision of the proposed algorithm mainly depends on the execution time
693 prediction model defined in (\ref{eq:perf}) and the energy model computed by
694 (\ref{eq:energy}). The energy model is also significantly dependent on the
695 execution time model because the static energy is linearly related to the
696 execution time and the dynamic energy is related to the computation time. So,
697 all the works presented in this paper are based on the execution time model. To
698 verify this model, the predicted execution time was compared to the real
699 execution time over SimGrid/SMPI simulator,
700 v3.10~\cite{casanova+giersch+legrand+al.2014.versatile}, for all the NAS
701 parallel benchmarks NPB v3.3 \cite{NAS.Parallel.Benchmarks}, running class B on
702 8 or 9 nodes. The comparison showed that the proposed execution time model is
703 very precise, the maximum normalized difference between the predicted execution
704 time and the real execution time is equal to 0.03 for all the NAS benchmarks.
706 Since the proposed algorithm is not an exact method it does not test all the
707 possible solutions (vectors of scaling factors) in the search space. To prove
708 its efficiency, it was compared on small instances to a brute force search
709 algorithm that tests all the possible solutions. The brute force algorithm was
710 applied to different NAS benchmarks classes with different number of nodes. The
711 solutions returned by the brute force algorithm and the proposed algorithm were
712 identical and the proposed algorithm was on average 10 times faster than the
713 brute force algorithm. It has a small execution time: for a heterogeneous
714 cluster composed of four different types of nodes having the characteristics
715 presented in Table~\ref{table:platform}, it takes on average \np[ms]{0.04} for 4
716 nodes and \np[ms]{0.15} on average for 144 nodes to compute the best scaling
717 factors vector. The algorithm complexity is $O(F\cdot (N \cdot4) )$, where $F$
718 is the number of iterations and $N$ is the number of computing nodes. The
719 algorithm needs from 12 to 20 iterations to select the best vector of frequency
720 scaling factors that gives the results of the next sections.
722 \section{Experimental results}
724 To evaluate the efficiency and the overall energy consumption reduction of
725 Algorithm~\ref{HSA}, it was applied to the NAS parallel benchmarks NPB v3.3. The
726 experiments were executed on the simulator SimGrid/SMPI which offers easy tools
727 to create a heterogeneous platform and run message passing applications over it.
728 The heterogeneous platform that was used in the experiments, had one core per
729 node because just one process was executed per node. The heterogeneous platform
730 was composed of four types of nodes. Each type of nodes had different
731 characteristics such as the maximum CPU frequency, the number of available
732 frequencies and the computational power, see Table~\ref{table:platform}. The
733 characteristics of these different types of nodes are inspired from the
734 specifications of real Intel processors. The heterogeneous platform had up to
735 144 nodes and had nodes from the four types in equal proportions, for example if
736 a benchmark was executed on 8 nodes, 2 nodes from each type were used. Since the
737 constructors of CPUs do not specify the dynamic and the static power of their
738 CPUs, for each type of node they were chosen proportionally to its computing
739 power (FLOPS). In the initial heterogeneous platform, while computing with
740 highest frequency, each node consumed an amount of power proportional to its
741 computing power (which corresponds to 80\% of its dynamic power and the
742 remaining 20\% to the static power), the same assumption was made in
743 \cite{Our_first_paper,Rauber_Analytical.Modeling.for.Energy}. Finally, These
744 nodes were connected via an Ethernet network with 1 Gbit/s bandwidth.
748 \caption{Heterogeneous nodes characteristics}
751 \begin{tabular}{|*{7}{l|}}
753 Node &Simulated & Max & Min & Diff. & Dynamic & Static \\
754 type &GFLOPS & Freq. & Freq. & Freq. & power & power \\
755 & & GHz & GHz &GHz & & \\
757 1 &40 & 2.5 & 1.2 & 0.1 & 20~W &4~W \\
760 2 &50 & 2.66 & 1.6 & 0.133 & 25~W &5~W \\
763 3 &60 & 2.9 & 1.2 & 0.1 & 30~W &6~W \\
766 4 &70 & 3.4 & 1.6 & 0.133 & 35~W &7~W \\
770 \label{table:platform}
774 %\subsection{Performance prediction verification}
777 \subsection{The experimental results of the scaling algorithm}
781 The proposed algorithm was applied to the seven parallel NAS benchmarks (EP, CG,
782 MG, FT, BT, LU and SP) and the benchmarks were executed with the three classes:
783 A, B and C. However, due to the lack of space in this paper, only the results of
784 the biggest class, C, are presented while being run on different number of
785 nodes, ranging from 4 to 128 or 144 nodes depending on the benchmark being
786 executed. Indeed, the benchmarks CG, MG, LU, EP and FT had to be executed on $1,
787 2, 4, 8, 16, 32, 64, 128$ nodes. The other benchmarks such as BT and SP had to
788 be executed on $1, 4, 9, 16, 36, 64, 144$ nodes.
793 \caption{Running NAS benchmarks on 4 nodes }
796 \begin{tabular}{|*{7}{r|}}
799 Program & Execution & Energy & Energy & Performance & Distance \\
800 name & time/s & consumption/J & saving\% & degradation\% & \\
802 CG & 64.64 & 3560.39 &34.16 &6.72 &27.44 \\
804 MG & 18.89 & 1074.87 &35.37 &4.34 &31.03 \\
806 EP &79.73 &5521.04 &26.83 &3.04 &23.79 \\
808 LU &308.65 &21126.00 &34.00 &6.16 &27.84 \\
810 BT &360.12 &21505.55 &35.36 &8.49 &26.87 \\
812 SP &234.24 &13572.16 &35.22 &5.70 &29.52 \\
814 FT &81.58 &4151.48 &35.58 &0.99 &34.59 \\
822 \caption{Running NAS benchmarks on 8 and 9 nodes }
825 \begin{tabular}{|*{7}{r|}}
828 Program & Execution & Energy & Energy & Performance & Distance \\
829 name & time/s & consumption/J & saving\% & degradation\% & \\
831 CG &36.11 &3263.49 &31.25 &7.12 &24.13 \\
833 MG &8.99 &953.39 &33.78 &6.41 &27.37 \\
835 EP &40.39 &5652.81 &27.04 &0.49 &26.55 \\
837 LU &218.79 &36149.77 &28.23 &0.01 &28.22 \\
839 BT &166.89 &23207.42 &32.32 &7.89 &24.43 \\
841 SP &104.73 &18414.62 &24.73 &2.78 &21.95 \\
843 FT &51.10 &4913.26 &31.02 &2.54 &28.48 \\
851 \caption{Running NAS benchmarks on 16 nodes }
854 \begin{tabular}{|*{7}{r|}}
857 Program & Execution & Energy & Energy & Performance & Distance \\
858 name & time/s & consumption/J & saving\% & degradation\% & \\
860 CG &31.74 &4373.90 &26.29 &9.57 &16.72 \\
862 MG &5.71 &1076.19 &32.49 &6.05 &26.44 \\
864 EP &20.11 &5638.49 &26.85 &0.56 &26.29 \\
866 LU &144.13 &42529.06 &28.80 &6.56 &22.24 \\
868 BT &97.29 &22813.86 &34.95 &5.80 &29.15 \\
870 SP &66.49 &20821.67 &22.49 &3.82 &18.67 \\
872 FT &37.01 &5505.60 &31.59 &6.48 &25.11 \\
875 \label{table:res_16n}
880 \caption{Running NAS benchmarks on 32 and 36 nodes }
883 \begin{tabular}{|*{7}{r|}}
886 Program & Execution & Energy & Energy & Performance & Distance \\
887 name & time/s & consumption/J & saving\% & degradation\% & \\
889 CG &32.35 &6704.21 &16.15 &5.30 &10.85 \\
891 MG &4.30 &1355.58 &28.93 &8.85 &20.08 \\
893 EP &9.96 &5519.68 &26.98 &0.02 &26.96 \\
895 LU &99.93 &67463.43 &23.60 &2.45 &21.15 \\
897 BT &48.61 &23796.97 &34.62 &5.83 &28.79 \\
899 SP &46.01 &27007.43 &22.72 &3.45 &19.27 \\
901 FT &28.06 &7142.69 &23.09 &2.90 &20.19 \\
904 \label{table:res_32n}
909 \caption{Running NAS benchmarks on 64 nodes }
912 \begin{tabular}{|*{7}{r|}}
915 Program & Execution & Energy & Energy & Performance & Distance \\
916 name & time/s & consumption/J & saving\% & degradation\% & \\
918 CG &46.65 &17521.83 &8.13 &1.68 &6.45 \\
920 MG &3.27 &1534.70 &29.27 &14.35 &14.92 \\
922 EP &5.05 &5471.1084 &27.12 &3.11 &24.01 \\
924 LU &73.92 &101339.16 &21.96 &3.67 &18.29 \\
926 BT &39.99 &27166.71 &32.02 &12.28 &19.74 \\
928 SP &52.00 &49099.28 &24.84 &0.03 &24.81 \\
930 FT &25.97 &10416.82 &20.15 &4.87 &15.28 \\
933 \label{table:res_64n}
938 \caption{Running NAS benchmarks on 128 and 144 nodes }
941 \begin{tabular}{|*{7}{r|}}
944 Program & Execution & Energy & Energy & Performance & Distance \\
945 name & time/s & consumption/J & saving\% & degradation\% & \\
947 CG &56.92 &41163.36 &4.00 &1.10 &2.90 \\
949 MG &3.55 &2843.33 &18.77 &10.38 &8.39 \\
951 EP &2.67 &5669.66 &27.09 &0.03 &27.06 \\
953 LU &51.23 &144471.90 &16.67 &2.36 &14.31 \\
955 BT &37.96 &44243.82 &23.18 &1.28 &21.90 \\
957 SP &64.53 &115409.71 &26.72 &0.05 &26.67 \\
959 FT &25.51 &18808.72 &12.85 &2.84 &10.01 \\
962 \label{table:res_128n}
964 The overall energy consumption was computed for each instance according to the
965 energy consumption model (\ref{eq:energy}), with and without applying the
966 algorithm. The execution time was also measured for all these experiments. Then,
967 the energy saving and performance degradation percentages were computed for each
968 instance. The results are presented in Tables~\ref{table:res_4n},
969 \ref{table:res_8n}, \ref{table:res_16n}, \ref{table:res_32n},
970 \ref{table:res_64n} and \ref{table:res_128n}. All these results are the average
971 values from many experiments for energy savings and performance degradation.
972 The tables show the experimental results for running the NAS parallel benchmarks
973 on different number of nodes. The experiments show that the algorithm
974 significantly reduces the energy consumption (up to 35\%) and tries to limit the
975 performance degradation. They also show that the energy saving percentage
976 decreases when the number of computing nodes increases. This reduction is due
977 to the increase of the communication times compared to the execution times when
978 the benchmarks are run over a high number of nodes. Indeed, the benchmarks with
979 the same class, C, are executed on different numbers of nodes, so the
980 computation required for each iteration is divided by the number of computing
981 nodes. On the other hand, more communications are required when increasing the
982 number of nodes so the static energy increases linearly according to the
983 communication time and the dynamic power is less relevant in the overall energy
984 consumption. Therefore, reducing the frequency with Algorithm~\ref{HSA} is
985 less effective in reducing the overall energy savings. It can also be noticed
986 that for the benchmarks EP and SP that contain little or no communications, the
987 energy savings are not significantly affected by the high number of nodes. No
988 experiments were conducted using bigger classes than D, because they require a
989 lot of memory (more than 64GB) when being executed by the simulator on one
990 machine. The maximum distance between the normalized energy curve and the
991 normalized performance for each instance is also shown in the result tables. It
992 decrease in the same way as the energy saving percentage. The tables also show
993 that the performance degradation percentage is not significantly increased when
994 the number of computing nodes is increased because the computation times are
995 small when compared to the communication times.
1001 \subfloat[Energy saving]{%
1002 \includegraphics[width=.33\textwidth]{fig/energy}\label{fig:energy}}%
1004 \subfloat[Performance degradation ]{%
1005 \includegraphics[width=.33\textwidth]{fig/per_deg}\label{fig:per_deg}}
1007 \caption{The energy and performance for all NAS benchmarks running with a different number of nodes}
1010 Figures~\ref{fig:energy} and \ref{fig:per_deg} present the energy saving and
1011 performance degradation respectively for all the benchmarks according to the
1012 number of used nodes. As shown in the first plot, the energy saving percentages
1013 of the benchmarks MG, LU, BT and FT decrease linearly when the number of nodes
1014 increase. While for the EP and SP benchmarks, the energy saving percentage is
1015 not affected by the increase of the number of computing nodes, because in these
1016 benchmarks there are little or no communications. Finally, the energy saving of
1017 the GC benchmark significantly decrease when the number of nodes increase
1018 because this benchmark has more communications than the others. The second plot
1019 shows that the performance degradation percentages of most of the benchmarks
1020 decrease when they run on a big number of nodes because they spend more time
1021 communicating than computing, thus, scaling down the frequencies of some nodes
1022 has less effect on the performance.
1027 \subsection{The results for different power consumption scenarios}
1029 The results of the previous section were obtained while using processors that
1030 consume during computation an overall power which is 80\% composed of dynamic
1031 power and of 20\% of static power. In this section, these ratios are changed and
1032 two new power scenarios are considered in order to evaluate how the proposed
1033 algorithm adapts itself according to the static and dynamic power values. The
1034 two new power scenarios are the following:
1037 \item 70\% of dynamic power and 30\% of static power
1038 \item 90\% of dynamic power and 10\% of static power
1041 The NAS parallel benchmarks were executed again over processors that follow the
1042 new power scenarios. The class C of each benchmark was run over 8 or 9 nodes
1043 and the results are presented in Tables~\ref{table:res_s1} and
1044 \ref{table:res_s2}. These tables show that the energy saving percentage of the
1045 70\%-30\% scenario is smaller for all benchmarks compared to the energy saving
1046 of the 90\%-10\% scenario. Indeed, in the latter more dynamic power is consumed
1047 when nodes are running on their maximum frequencies, thus, scaling down the
1048 frequency of the nodes results in higher energy savings than in the 70\%-30\%
1049 scenario. On the other hand, the performance degradation percentage is smaller
1050 in the 70\%-30\% scenario compared to the 90\%-10\% scenario. This is due to the
1051 higher static power percentage in the first scenario which makes it more
1052 relevant in the overall consumed energy. Indeed, the static energy is related
1053 to the execution time and if the performance is degraded the amount of consumed
1054 static energy directly increases. Therefore, the proposed algorithm does not
1055 really significantly scale down much the frequencies of the nodes in order to
1056 limit the increase of the execution time and thus limiting the effect of the
1057 consumed static energy.
1059 Both new power scenarios are compared to the old one in
1060 Figure~\ref{fig:sen_comp}. It shows the average of the performance degradation, the
1061 energy saving and the distances for all NAS benchmarks of class C running on 8
1062 or 9 nodes. The comparison shows that the energy saving ratio is proportional
1063 to the dynamic power ratio: it is increased when applying the 90\%-10\% scenario
1064 because at maximum frequency the dynamic energy is the most relevant in the
1065 overall consumed energy and can be reduced by lowering the frequency of some
1066 processors. On the other hand, the energy saving decreases when the 70\%-30\%
1067 scenario is used because the dynamic energy is less relevant in the overall
1068 consumed energy and lowering the frequency does not return big energy savings.
1069 Moreover, the average of the performance degradation is decreased when using a
1070 higher ratio for static power (e.g. 70\%-30\% scenario and 80\%-20\%
1071 scenario). Since the proposed algorithm optimizes the energy consumption when
1072 using a higher ratio for dynamic power the algorithm selects bigger frequency
1073 scaling factors that result in more energy saving but less performance, for
1074 example see Figure~\ref{fig:scales_comp}. The opposite happens when using a
1075 higher ratio for static power, the algorithm proportionally selects smaller
1076 scaling values which result in less energy saving but also less performance
1081 \caption{The results of the 70\%-30\% power scenario}
1084 \begin{tabular}{|*{6}{r|}}
1086 Program & Energy & Energy & Performance & Distance \\
1087 name & consumption/J & saving\% & degradation\% & \\
1089 CG &4144.21 &22.42 &7.72 &14.70 \\
1091 MG &1133.23 &24.50 &5.34 &19.16 \\
1093 EP &6170.30 &16.19 &0.02 &16.17 \\
1095 LU &39477.28 &20.43 &0.07 &20.36 \\
1097 BT &26169.55 &25.34 &6.62 &18.71 \\
1099 SP &19620.09 &19.32 &3.66 &15.66 \\
1101 FT &6094.07 &23.17 &0.36 &22.81 \\
1104 \label{table:res_s1}
1110 \caption{The results of the 90\%-10\% power scenario}
1113 \begin{tabular}{|*{6}{r|}}
1115 Program & Energy & Energy & Performance & Distance \\
1116 name & consumption/J & saving\% & degradation\% & \\
1118 CG &2812.38 &36.36 &6.80 &29.56 \\
1120 MG &825.427 &38.35 &6.41 &31.94 \\
1122 EP &5281.62 &35.02 &2.68 &32.34 \\
1124 LU &31611.28 &39.15 &3.51 &35.64 \\
1126 BT &21296.46 &36.70 &6.60 &30.10 \\
1128 SP &15183.42 &35.19 &11.76 &23.43 \\
1130 FT &3856.54 &40.80 &5.67 &35.13 \\
1133 \label{table:res_s2}
1137 \caption{Comparing the proposed algorithm}
1139 \begin{tabular}{|*{7}{r|}}
1141 Program & \multicolumn{2}{c|}{Energy saving \%} & \multicolumn{2}{c|}{Perf. degradation \%} & \multicolumn{2}{c|}{Distance} \\ \cline{2-7}
1142 name & EDP & MaxDist & EDP & MaxDist & EDP & MaxDist \\ \hline
1143 CG & 27.58 & 31.25 & 5.82 & 7.12 & 21.76 & 24.13 \\ \hline
1144 MG & 29.49 & 33.78 & 3.74 & 6.41 & 25.75 & 27.37 \\ \hline
1145 LU & 19.55 & 28.33 & 0.0 & 0.01 & 19.55 & 28.22 \\ \hline
1146 EP & 28.40 & 27.04 & 4.29 & 0.49 & 24.11 & 26.55 \\ \hline
1147 BT & 27.68 & 32.32 & 6.45 & 7.87 & 21.23 & 24.43 \\ \hline
1148 SP & 20.52 & 24.73 & 5.21 & 2.78 & 15.31 & 21.95 \\ \hline
1149 FT & 27.03 & 31.02 & 2.75 & 2.54 & 24.28 & 28.48 \\ \hline
1152 \label{table:compare_EDP}
1157 \subfloat[Comparison between the results on 8 nodes]{%
1158 \includegraphics[width=.33\textwidth]{fig/sen_comp}\label{fig:sen_comp}}%
1160 \subfloat[Comparison the selected frequency scaling factors of MG benchmark class C running on 8 nodes]{%
1161 \includegraphics[width=.33\textwidth]{fig/three_scenarios}\label{fig:scales_comp}}
1163 \caption{The comparison of the three power scenarios}
1168 \includegraphics[scale=0.5]{fig/compare_EDP.pdf}
1169 \caption{Trade-off comparison for NAS benchmarks class C}
1170 \label{fig:compare_EDP}
1174 \subsection{The comparison of the proposed scaling algorithm }
1175 \label{sec.compare_EDP}
1176 In this section, the scaling factors selection algorithm, called MaxDist, is
1177 compared to Spiliopoulos et al. algorithm
1178 \cite{Spiliopoulos_Green.governors.Adaptive.DVFS}, called EDP. They developed a
1179 green governor that regularly applies an online frequency selecting algorithm to
1180 reduce the energy consumed by a multicore architecture without degrading much
1181 its performance. The algorithm selects the frequencies that minimize the energy
1182 and delay products, $\mathit{EDP}=\mathit{energy}\times \mathit{delay}$ using
1183 the predicted overall energy consumption and execution time delay for each
1184 frequency. To fairly compare both algorithms, the same energy and execution
1185 time models, equations (\ref{eq:energy}) and (\ref{eq:fnew}), were used for both
1186 algorithms to predict the energy consumption and the execution times. Also
1187 Spiliopoulos et al. algorithm was adapted to start the search from the initial
1188 frequencies computed using the equation (\ref{eq:Fint}). The resulting algorithm
1189 is an exhaustive search algorithm that minimizes the EDP and has the initial
1190 frequencies values as an upper bound.
1192 Both algorithms were applied to the parallel NAS benchmarks to compare their
1193 efficiency. Table~\ref{table:compare_EDP} presents the results of comparing the
1194 execution times and the energy consumption for both versions of the NAS
1195 benchmarks while running the class C of each benchmark over 8 or 9 heterogeneous
1196 nodes. The results show that our algorithm provides better energy savings than
1197 Spiliopoulos et al. algorithm, on average it results in 29.76\% energy saving
1198 while their algorithm returns just 25.75\%. The average of performance
1199 degradation percentage is approximately the same for both algorithms, about 4\%.
1202 For all benchmarks, our algorithm outperforms Spiliopoulos et al. algorithm in
1203 terms of energy and performance trade-off, see Figure~\ref{fig:compare_EDP},
1204 because it maximizes the distance between the energy saving and the performance
1205 degradation values while giving the same weight for both metrics.
1208 \section{Conclusion}
1210 In this paper, a new online frequency selecting algorithm has been presented. It
1211 selects the best possible vector of frequency scaling factors that gives the
1212 maximum distance (optimal trade-off) between the predicted energy and the
1213 predicted performance curves for a heterogeneous platform. This algorithm uses a
1214 new energy model for measuring and predicting the energy of distributed
1215 iterative applications running over heterogeneous platforms. To evaluate the
1216 proposed method, it was applied on the NAS parallel benchmarks and executed over
1217 a heterogeneous platform simulated by SimGrid. The results of the experiments
1218 showed that the algorithm reduces up to 35\% the energy consumption of a message
1219 passing iterative method while limiting the degradation of the performance. The
1220 algorithm also selects different scaling factors according to the percentage of
1221 the computing and communication times, and according to the values of the static
1222 and dynamic powers of the CPUs. Finally, the algorithm was compared to
1223 Spiliopoulos et al. algorithm and the results showed that it outperforms their
1224 algorithm in terms of energy-time trade-off.
1226 In the near future, this method will be applied to real heterogeneous platforms
1227 to evaluate its performance in a real study case. It would also be interesting
1228 to evaluate its scalability over large scale heterogeneous platforms and measure
1229 the energy consumption reduction it can produce. Afterward, we would like to
1230 develop a similar method that is adapted to asynchronous iterative applications
1231 where each task does not wait for other tasks to finish their works. The
1232 development of such a method might require a new energy model because the number
1233 of iterations is not known in advance and depends on the global convergence of
1234 the iterative system.
1236 \section*{Acknowledgment}
1238 This work has been partially supported by the Labex
1239 ACTION project (contract “ANR-11-LABX-01-01”). As a PhD student,
1240 Mr. Ahmed Fanfakh, would like to thank the University of
1241 Babylon (Iraq) for supporting his work.
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