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68 \title{Energy Consumption Reduction for Message Passing Iterative Applications in Heterogeneous Architecture Using DVFS}
78 FEMTO-ST Institute, University of Franche-Comte\\
79 IUT de Belfort-Montbéliard,
80 19 avenue du Maréchal Juin, BP 527, 90016 Belfort cedex, France\\
81 % Telephone: \mbox{+33 3 84 58 77 86}, % Raphaël
82 % Fax: \mbox{+33 3 84 58 77 81}\\ % Dept Info
83 Email: \email{{jean-claude.charr,raphael.couturier,ahmed.fanfakh_badri_muslim,arnaud.giersch}@univ-fcomte.fr}
90 Computing platforms are consuming more and more energy due to the increasing
91 number of nodes composing them. To minimize the operating costs of these
92 platforms many techniques have been used. Dynamic voltage and frequency scaling
93 (DVFS) is one of them. It reduces the frequency of a CPU to lower its energy
94 consumption. However, lowering the frequency of a CPU might increase the
95 execution time of an application running on that processor. Therefore, the
96 frequency that gives the best trade-off between the energy consumption and the
97 performance of an application must be selected.\\
98 In this paper, a new online frequencies selecting algorithm for heterogeneous
99 platforms is presented. It selects the frequency which tries to give the best
100 trade-off between energy saving and performance degradation, for each node
101 computing the message passing iterative application. The algorithm has a small
102 overhead and works without training or profiling. It uses a new energy model for
103 message passing iterative applications running on a heterogeneous platform. The
104 proposed algorithm is evaluated on the SimGrid simulator while running the NAS
105 parallel benchmarks. The experiments show that it reduces the energy
106 consumption by up to 35\% while limiting the performance degradation as much as
107 possible. Finally, the algorithm is compared to an existing method, the
108 comparison results showing that it outperforms the latter.
112 \section{Introduction}
114 The need for more computing power is continually increasing. To partially
115 satisfy this need, most supercomputers constructors just put more computing
116 nodes in their platform. The resulting platforms might achieve higher floating
117 point operations per second (FLOPS), but the energy consumption and the heat
118 dissipation are also increased. As an example, the Chinese supercomputer
119 Tianhe-2 had the highest FLOPS in November 2014 according to the Top500 list
120 \cite{TOP500_Supercomputers_Sites}. However, it was also the most power hungry
121 platform with its over 3 million cores consuming around 17.8 megawatts.
122 Moreover, according to the U.S. annual energy outlook 2014
123 \cite{U.S_Annual.Energy.Outlook.2014}, the price of energy for 1 megawatt-hour
124 was approximately equal to \$70. Therefore, the price of the energy consumed by
125 the Tianhe-2 platform is approximately more than \$10 million each year. The
126 computing platforms must be more energy efficient and offer the highest number
127 of FLOPS per watt possible, such as the L-CSC from the GSI Helmholtz Center
128 which became the top of the Green500 list in November 2014 \cite{Green500_List}.
129 This heterogeneous platform executes more than 5 GFLOPS per watt while consuming
132 Besides platform improvements, there are many software and hardware techniques
133 to lower the energy consumption of these platforms, such as scheduling, DVFS,
134 \dots{} DVFS is a widely used process to reduce the energy consumption of a
135 processor by lowering its frequency
136 \cite{Rizvandi_Some.Observations.on.Optimal.Frequency}. However, it also reduces
137 the number of FLOPS executed by the processor which might increase the execution
138 time of the application running over that processor. Therefore, researchers use
139 different optimization strategies to select the frequency that gives the best
140 trade-off between the energy reduction and performance degradation ratio. In
141 \cite{Our_first_paper}, a frequency selecting algorithm was proposed to reduce
142 the energy consumption of message passing iterative applications running over
143 homogeneous platforms. The results of the experiments show significant energy
144 consumption reductions. In this paper, a new frequency selecting algorithm
145 adapted for heterogeneous platform is presented. It selects the vector of
146 frequencies, for a heterogeneous platform running a message passing iterative
147 application, that simultaneously tries to offer the maximum energy reduction and
148 minimum performance degradation ratio. The algorithm has a very small overhead,
149 works online and does not need any training or profiling.
151 This paper is organized as follows: Section~\ref{sec.relwork} presents some
152 related works from other authors. Section~\ref{sec.exe} describes how the
153 execution time of message passing programs can be predicted. It also presents an energy
154 model that predicts the energy consumption of an application running over a heterogeneous platform. Section~\ref{sec.compet} presents
155 the energy-performance objective function that maximizes the reduction of energy
156 consumption while minimizing the degradation of the program's performance.
157 Section~\ref{sec.optim} details the proposed frequency selecting algorithm then the precision of the proposed algorithm is verified.
158 Section~\ref{sec.expe} presents the results of applying the algorithm on the NAS parallel benchmarks and executing them
159 on a heterogeneous platform. It shows the results of running three
160 different power scenarios and comparing them. Moreover, it also shows the comparison results
161 between the proposed method and an existing method.
162 Finally, in Section~\ref{sec.concl} the paper ends with a summary and some future works.
164 \section{Related works}
166 DVFS is a technique used in modern processors to scale down both the voltage and
167 the frequency of the CPU while computing, in order to reduce the energy
168 consumption of the processor. DVFS is also allowed in GPUs to achieve the same
169 goal. Reducing the frequency of a processor lowers its number of FLOPS and might
170 degrade the performance of the application running on that processor, especially
171 if it is compute bound. Therefore selecting the appropriate frequency for a
172 processor to satisfy some objectives while taking into account all the
173 constraints, is not a trivial operation. Many researchers used different
174 strategies to tackle this problem. Some of them developed online methods that
175 compute the new frequency while executing the application, such
176 as~\cite{Hao_Learning.based.DVFS,Spiliopoulos_Green.governors.Adaptive.DVFS}.
177 Others used offline methods that might need to run the application and profile
178 it before selecting the new frequency, such
179 as~\cite{Rountree_Bounding.energy.consumption.in.MPI,Cochran_Pack_and_Cap_Adaptive_DVFS}.
180 The methods could be heuristics, exact or brute force methods that satisfy
181 varied objectives such as energy reduction or performance. They also could be
182 adapted to the execution's environment and the type of the application such as
183 sequential, parallel or distributed architecture, homogeneous or heterogeneous
184 platform, synchronous or asynchronous application, \dots{}
186 In this paper, we are interested in reducing energy for message passing iterative synchronous applications running over heterogeneous platforms.
187 Some works have already been done for such platforms and they can be classified into two types of heterogeneous platforms:
190 \item the platform is composed of homogeneous GPUs and homogeneous CPUs.
191 \item the platform is only composed of heterogeneous CPUs.
195 For the first type of platform, the computing intensive parallel tasks are
196 executed on the GPUs and the rest are executed on the CPUs. Luley et
197 al.~\cite{Luley_Energy.efficiency.evaluation.and.benchmarking}, proposed a
198 heterogeneous cluster composed of Intel Xeon CPUs and NVIDIA GPUs. Their main
199 goal was to maximize the energy efficiency of the platform during computation by
200 maximizing the number of FLOPS per watt generated.
201 In~\cite{KaiMa_Holistic.Approach.to.Energy.Efficiency.in.GPU-CPU}, Kai Ma et
202 al. developed a scheduling algorithm that distributes workloads proportional to
203 the computing power of the nodes which could be a GPU or a CPU. All the tasks
204 must be completed at the same time. In~\cite{Rong_Effects.of.DVFS.on.K20.GPU},
205 Rong et al. showed that a heterogeneous (GPUs and CPUs) cluster that enables
206 DVFS gave better energy and performance efficiency than other clusters only
209 The work presented in this paper concerns the second type of platform, with
210 heterogeneous CPUs. Many methods were conceived to reduce the energy
211 consumption of this type of platform. Naveen et
212 al.~\cite{Naveen_Power.Efficient.Resource.Scaling} developed a method that
213 minimizes the value of $energy\cdot delay^2$ (the delay is the sum of slack
214 times that happen during synchronous communications) by dynamically assigning
215 new frequencies to the CPUs of the heterogeneous cluster. Lizhe et
216 al.~\cite{Lizhe_Energy.aware.parallel.task.scheduling} proposed an algorithm
217 that divides the executed tasks into two types: the critical and non critical
218 tasks. The algorithm scales down the frequency of non critical tasks
219 proportionally to their slack and communication times while limiting the
220 performance degradation percentage to less than
221 10\%. In~\cite{Joshi_Blackbox.prediction.of.impact.of.DVFS}, they developed a
222 heterogeneous cluster composed of two types of Intel and AMD processors. They
223 use a gradient method to predict the impact of DVFS operations on performance.
224 In~\cite{Shelepov_Scheduling.on.Heterogeneous.Multicore} and
225 \cite{Li_Minimizing.Energy.Consumption.for.Frame.Based.Tasks}, the best
226 frequencies for a specified heterogeneous cluster are selected offline using
227 some heuristic. Chen et
228 al.~\cite{Chen_DVFS.under.quality.of.service.requirements} used a greedy dynamic
229 programming approach to minimize the power consumption of heterogeneous servers
230 while respecting given time constraints. This approach had considerable
231 overhead. In contrast to the above described papers, this paper presents the
232 following contributions :
234 \item two new energy and performance models for message passing iterative synchronous applications running over
235 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.
237 \item a new online frequency selecting algorithm for heterogeneous platforms. The algorithm has a very small
238 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.
242 \section{The performance and energy consumption measurements on heterogeneous architecture}
247 \subsection{The execution time of message passing distributed
248 iterative applications on a heterogeneous platform}
250 In this paper, we are interested in reducing the energy consumption of message
251 passing distributed iterative synchronous applications running over
252 heterogeneous platforms. A heterogeneous platform is defined as a collection of
253 heterogeneous computing nodes interconnected via a high speed homogeneous
254 network. Therefore, each node has different characteristics such as computing
255 power (FLOPS), energy consumption, CPU's frequency range, \dots{} but they all
256 have the same network bandwidth and latency.
258 The overall execution time of a distributed iterative synchronous application
259 over a heterogeneous platform consists of the sum of the computation time and
260 the communication time for every iteration on a node. However, due to the
261 heterogeneous computation power of the computing nodes, slack times might occur
262 when fast nodes have to wait, during synchronous communications, for the slower
263 nodes to finish their computations (see Figure~\ref{fig:heter}). Therefore, the
264 overall execution time of the program is the execution time of the slowest task
265 which has the highest computation time and no slack time.
269 \includegraphics[scale=0.6]{fig/commtasks}
270 \caption{Parallel tasks on a heterogeneous platform}
274 Dynamic Voltage and Frequency Scaling (DVFS) is a process, implemented in
275 modern processors, that reduces the energy consumption of a CPU by scaling
276 down its voltage and frequency. Since DVFS lowers the frequency of a CPU
277 and consequently its computing power, the execution time of a program running
278 over that scaled down processor might increase, especially if the program is
279 compute bound. The frequency reduction process can be expressed by the scaling
280 factor S which is the ratio between the maximum and the new frequency of a CPU
284 S = \frac{\Fmax}{\Fnew}
286 The execution time of a compute bound sequential program is linearly proportional
287 to the frequency scaling factor $S$. On the other hand, message passing
288 distributed applications consist of two parts: computation and communication.
289 The execution time of the computation part is linearly proportional to the
290 frequency scaling factor $S$ but the communication time is not affected by the
291 scaling factor because the processors involved remain idle during the
292 communications~\cite{Freeh_Exploring.the.Energy.Time.Tradeoff}.
293 The communication time for a task is the summation of periods of
294 time that begin with an MPI call for sending or receiving a message
295 until the message is synchronously sent or received.
297 Since in a heterogeneous platform each node has different characteristics,
298 especially different frequency gears, when applying DVFS operations on these
299 nodes, they may get different scaling factors represented by a scaling vector:
300 $(S_1, S_2,\dots, S_N)$ where $S_i$ is the scaling factor of processor $i$. To
301 be able to predict the execution time of message passing synchronous iterative
302 applications running over a heterogeneous platform, for different vectors of
303 scaling factors, the communication time and the computation time for all the
304 tasks must be measured during the first iteration before applying any DVFS
305 operation. Then the execution time for one iteration of the application with any
306 vector of scaling factors can be predicted using (\ref{eq:perf}).
309 \Tnew = \max_{i=1,2,\dots,N} ({\TcpOld_{i}} \cdot S_{i}) + \MinTcm
314 \MinTcm = \min_{i=1,2,\dots,N} (\Tcm_i)
316 where $\TcpOld_i$ is the computation time of processor $i$ during the first
317 iteration and $\MinTcm$ is the communication time of the slowest processor from
318 the first iteration. The model computes the maximum computation time with
319 scaling factor from each node added to the communication time of the slowest
320 node. It means only the communication time without any slack time is taken into
321 account. Therefore, the execution time of the iterative application is equal to
322 the execution time of one iteration as in (\ref{eq:perf}) multiplied by the
323 number of iterations of that application.
325 This prediction model is developed from the model to predict the execution time
326 of message passing distributed applications for homogeneous
327 architectures~\cite{Our_first_paper}. The execution time prediction model is
328 used in the method to optimize both the energy consumption and the performance of
329 iterative methods, which is presented in the following sections.
332 \subsection{Energy model for heterogeneous platform}
333 Many researchers~\cite{Malkowski_energy.efficient.high.performance.computing,
334 Rauber_Analytical.Modeling.for.Energy,Zhuo_Energy.efficient.Dynamic.Task.Scheduling,
335 Rizvandi_Some.Observations.on.Optimal.Frequency} divide the power consumed by a processor into
336 two power metrics: the static and the dynamic power. While the first one is
337 consumed as long as the computing unit is turned on, the latter is only consumed during
338 computation times. The dynamic power $\Pd$ is related to the switching
339 activity $\alpha$, load capacitance $\CL$, the supply voltage $V$ and
340 operational frequency $F$, as shown in (\ref{eq:pd}).
343 \Pd = \alpha \cdot \CL \cdot V^2 \cdot F
345 The static power $\Ps$ captures the leakage power as follows:
348 \Ps = V \cdot \Ntrans \cdot \Kdesign \cdot \Ileak
350 where V is the supply voltage, $\Ntrans$ is the number of transistors,
351 $\Kdesign$ is a design dependent parameter and $\Ileak$ is a
352 technology dependent parameter. The energy consumed by an individual processor
353 to execute a given program can be computed as:
356 \Eind = \Pd \cdot \Tcp + \Ps \cdot T
358 where $T$ is the execution time of the program, $\Tcp$ is the computation
359 time and $\Tcp \le T$. $\Tcp$ may be equal to $T$ if there is no
360 communication and no slack time.
362 The main objective of DVFS operation is to reduce the overall energy consumption~\cite{Le_DVFS.Laws.of.Diminishing.Returns}.
363 The operational frequency $F$ depends linearly on the supply voltage $V$, i.e., $V = \beta \cdot F$ with some
364 constant $\beta$.~This equation is used to study the change of the dynamic
365 voltage with respect to various frequency values in~\cite{Rauber_Analytical.Modeling.for.Energy}. The reduction
366 process of the frequency can be expressed by the scaling factor $S$ which is the
367 ratio between the maximum and the new frequency as in (\ref{eq:s}).
368 The CPU governors are power schemes supplied by the operating
369 system's kernel to lower a core's frequency. The new frequency
370 $\Fnew$ from (\ref{eq:s}) can be calculated as follows:
373 \Fnew = S^{-1} \cdot \Fmax
375 Replacing $\Fnew$ in (\ref{eq:pd}) as in (\ref{eq:fnew}) gives the following
376 equation for dynamic power consumption:
379 \PdNew = \alpha \cdot \CL \cdot V^2 \cdot \Fnew = \alpha \cdot \CL \cdot \beta^2 \cdot \Fnew^3 \\
380 {} = \alpha \cdot \CL \cdot V^2 \cdot \Fmax \cdot S^{-3} = \PdOld \cdot S^{-3}
382 where $\PdNew$ and $\PdOld$ are the dynamic power consumed with the
383 new frequency and the maximum frequency respectively.
385 According to (\ref{eq:pdnew}) the dynamic power is reduced by a factor of $S^{-3}$ when
386 reducing the frequency by a factor of $S$~\cite{Rauber_Analytical.Modeling.for.Energy}. Since the FLOPS of a CPU is proportional
387 to the frequency of a CPU, the computation time is increased proportionally to $S$.
388 The new dynamic energy is the dynamic power multiplied by the new time of computation
389 and is given by the following equation:
392 \EdNew = \PdOld \cdot S^{-3} \cdot (\Tcp \cdot S)= S^{-2}\cdot \PdOld \cdot \Tcp
394 The static power is related to the power leakage of the CPU and is consumed during computation
395 and even when idle. As in~\cite{Rauber_Analytical.Modeling.for.Energy,Zhuo_Energy.efficient.Dynamic.Task.Scheduling},
396 the static power of a processor is considered as constant
397 during idle and computation periods, and for all its available frequencies.
398 The static energy is the static power multiplied by the execution time of the program.
399 According to the execution time model in (\ref{eq:perf}), the execution time of the program
400 is the sum of the computation and the communication times. The computation time is linearly related
401 to the frequency scaling factor, while this scaling factor does not affect the communication time.
402 The static energy of a processor after scaling its frequency is computed as follows:
405 \Es = \Ps \cdot (\Tcp \cdot S + \Tcm)
408 In the considered heterogeneous platform, each processor $i$ might have
409 different dynamic and static powers, noted as $\Pd_{i}$ and $\Ps_{i}$
410 respectively. Therefore, even if the distributed message passing iterative
411 application is load balanced, the computation time of each CPU $i$ noted
412 $\Tcp_{i}$ might be different and different frequency scaling factors might be
413 computed in order to decrease the overall energy consumption of the application
414 and reduce slack times. The communication time of a processor $i$ is noted as
415 $\Tcm_{i}$ and could contain slack times when communicating with slower
416 nodes, see Figure~\ref{fig:heter}. Therefore, all nodes do not have equal
417 communication times. While the dynamic energy is computed according to the
418 frequency scaling factor and the dynamic power of each node as in
419 (\ref{eq:Edyn}), the static energy is computed as the sum of the execution time
420 of one iteration multiplied by the static power of each processor. The overall
421 energy consumption of a message passing distributed application executed over a
422 heterogeneous platform during one iteration is the summation of all dynamic and
423 static energies for each processor. It is computed as follows:
426 E = \sum_{i=1}^{N} {(S_i^{-2} \cdot \Pd_{i} \cdot \Tcp_i)} + {} \\
427 \sum_{i=1}^{N} (\Ps_{i} \cdot (\max_{i=1,2,\dots,N} (\Tcp_i \cdot S_{i}) +
431 Reducing the frequencies of the processors according to the vector of
432 scaling factors $(S_1, S_2,\dots, S_N)$ may degrade the performance of the
433 application and thus, increase the static energy because the execution time is
434 increased~\cite{Kim_Leakage.Current.Moore.Law}. The overall energy consumption for the iterative
435 application can be measured by measuring the energy consumption for one iteration as in (\ref{eq:energy})
436 multiplied by the number of iterations of that application.
439 \section{Optimization of both energy consumption and performance}
442 Using the lowest frequency for each processor does not necessarily give the most
443 energy efficient execution of an application. Indeed, even though the dynamic
444 power is reduced while scaling down the frequency of a processor, its
445 computation power is proportionally decreased. Hence, the execution time might
446 be drastically increased and during that time, dynamic and static powers are
447 being consumed. Therefore, it might cancel any gains achieved by scaling down
448 the frequency of all nodes to the minimum and the overall energy consumption of
449 the application might not be the optimal one. It is not trivial to select the
450 appropriate frequency scaling factor for each processor while considering the
451 characteristics of each processor (computation power, range of frequencies,
452 dynamic and static powers) and the task executed (computation/communication
453 ratio). The aim being to reduce the overall energy consumption and to avoid
454 increasing significantly the execution time. In our previous
455 work~\cite{Our_first_paper}, we proposed a method that selects the optimal
456 frequency scaling factor for a homogeneous cluster executing a message passing
457 iterative synchronous application while giving the best trade-off between the
458 energy consumption and the performance for such applications. In this work we
459 are interested in heterogeneous clusters as described above. Due to the
460 heterogeneity of the processors, a vector of scaling factors should
461 be selected and it must give the best trade-off between energy consumption and
464 The relation between the energy consumption and the execution time for an
465 application is complex and nonlinear, Thus, unlike the relation between the
466 execution time and the scaling factor, the relation between the energy and the
467 frequency scaling factors is nonlinear, for more details refer
468 to~\cite{Freeh_Exploring.the.Energy.Time.Tradeoff}. Moreover, these relations
469 are not measured using the same metric. To solve this problem, the execution
470 time is normalized by computing the ratio between the new execution time (after
471 scaling down the frequencies of some processors) and the initial one (with
472 maximum frequency for all nodes) as follows:
475 \Pnorm = \frac{\Tnew}{\Told}\\
476 {} = \frac{ \max_{i=1,2,\dots,N} (\Tcp_{i} \cdot S_{i}) +\MinTcm}
477 {\max_{i=1,2,\dots,N}{(\Tcp_i+\Tcm_i)}}
481 In the same way, the energy is normalized by computing the ratio between the consumed energy
482 while scaling down the frequency and the consumed energy with maximum frequency for all nodes:
485 \Enorm = \frac{\Ereduced}{\Eoriginal} \\
486 {} = \frac{ \sum_{i=1}^{N}{(S_i^{-2} \cdot \Pd_i \cdot \Tcp_i)} +
487 \sum_{i=1}^{N} {(\Ps_i \cdot \Tnew)}}{\sum_{i=1}^{N}{( \Pd_i \cdot \Tcp_i)} +
488 \sum_{i=1}^{N} {(\Ps_i \cdot \Told)}}
490 Where $\Ereduced$ and $\Eoriginal$ are computed using (\ref{eq:energy}) and
491 $\Tnew$ and $\Told$ are computed as in (\ref{eq:pnorm}).
494 goal is to optimize the energy and execution time at the same time, the normalized
495 energy and execution time curves are not in the same direction. According
496 to the equations~(\ref{eq:pnorm}) and (\ref{eq:enorm}), the vector of frequency
497 scaling factors $S_1,S_2,\dots,S_N$ reduce both the energy and the execution
498 time simultaneously. But the main objective is to produce maximum energy
499 reduction with minimum execution time reduction.
501 This problem can be solved by making the optimization process for energy and
502 execution time following the same direction. Therefore, the equation of the
503 normalized execution time is inverted which gives the normalized performance equation, as follows:
506 \Pnorm = \frac{\Told}{\Tnew}\\
507 = \frac{\max_{i=1,2,\dots,N}{(\Tcp_i+\Tcm_i)}}
508 { \max_{i=1,2,\dots,N} (\Tcp_{i} \cdot S_{i}) + \MinTcm}
514 \subfloat[Homogeneous platform]{%
515 \includegraphics[width=.33\textwidth]{fig/homo}\label{fig:r1}}%
518 \subfloat[Heterogeneous platform]{%
519 \includegraphics[width=.33\textwidth]{fig/heter}\label{fig:r2}}
521 \caption{The energy and performance relation}
524 Then, the objective function can be modeled in order to find the maximum
525 distance between the energy curve (\ref{eq:enorm}) and the performance curve
526 (\ref{eq:pnorm_inv}) over all available sets of scaling factors. This
527 represents the minimum energy consumption with minimum execution time (maximum
528 performance) at the same time, see Figure~\ref{fig:r1} or
529 Figure~\ref{fig:r2}. Then the objective function has the following form:
533 \mathop{\max_{i=1,\dots F}}_{j=1,\dots,N}
534 (\overbrace{\Pnorm(S_{ij})}^{\text{Maximize}} -
535 \overbrace{\Enorm(S_{ij})}^{\text{Minimize}} )
537 where $N$ is the number of nodes and $F$ is the number of available frequencies for each node.
538 Then, the optimal set of scaling factors that satisfies (\ref{eq:max}) can be selected.
539 The objective function can work with any energy model or any power values for each node
540 (static and dynamic powers). However, the most important energy reduction gain can be achieved when
541 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}.
543 \section{The scaling factors selection algorithm for heterogeneous platforms }
546 \subsection{The algorithm details}
547 In this section, Algorithm~\ref{HSA} is presented. It selects the frequency
548 scaling factors vector that gives the best trade-off between minimizing the
549 energy consumption and maximizing the performance of a message passing
550 synchronous iterative application executed on a heterogeneous platform. It works
551 online during the execution time of the iterative message passing program. It
552 uses information gathered during the first iteration such as the computation
553 time and the communication time in one iteration for each node. The algorithm is
554 executed after the first iteration and returns a vector of optimal frequency
555 scaling factors that satisfies the objective function (\ref{eq:max}). The
556 program applies DVFS operations to change the frequencies of the CPUs according
557 to the computed scaling factors. This algorithm is called just once during the
558 execution of the program. Algorithm~\ref{dvfs} shows where and when the proposed
559 scaling algorithm is called in the iterative MPI program.
561 The nodes in a heterogeneous platform have different computing powers, thus
562 while executing message passing iterative synchronous applications, fast nodes
563 have to wait for the slower ones to finish their computations before being able
564 to synchronously communicate with them as in Figure~\ref{fig:heter}. These
565 periods are called idle or slack times. The algorithm takes into account this
566 problem and tries to reduce these slack times when selecting the frequency
567 scaling factors vector. At first, it selects initial frequency scaling factors
568 that increase the execution times of fast nodes and minimize the differences
569 between the computation times of fast and slow nodes. The value of the initial
570 frequency scaling factor for each node is inversely proportional to its
571 computation time that was gathered from the first iteration. These initial
572 frequency scaling factors are computed as a ratio between the computation time
573 of the slowest node and the computation time of the node $i$ as follows:
576 \Scp_{i} = \frac{\max_{i=1,2,\dots,N}(\Tcp_i)}{\Tcp_i}
578 Using the initial frequency scaling factors computed in (\ref{eq:Scp}), the algorithm computes
579 the initial frequencies for all nodes as a ratio between the maximum frequency of node $i$
580 and the computation scaling factor $\Scp_i$ as follows:
583 F_{i} = \frac{\Fmax_i}{\Scp_i},~{i=1,2,\dots,N}
585 If the computed initial frequency for a node is not available in the gears of
586 that node, it is replaced by the nearest available frequency. In
587 Figure~\ref{fig:st_freq}, the nodes are sorted by their computing power in
588 ascending order and the frequencies of the faster nodes are scaled down
589 according to the computed initial frequency scaling factors. The resulting new
590 frequencies are colored in blue in Figure~\ref{fig:st_freq}. This set of
591 frequencies can be considered as a higher bound for the search space of the
592 optimal vector of frequencies because selecting frequency scaling factors higher
593 than the higher bound will not improve the performance of the application and it
594 will increase its overall energy consumption. Therefore the algorithm that
595 selects the frequency scaling factors starts the search method from these
596 initial frequencies and takes a downward search direction toward lower
597 frequencies. The algorithm iterates on all left frequencies, from the higher
598 bound until all nodes reach their minimum frequencies, to compute their overall
599 energy consumption and performance, and select the optimal frequency scaling
600 factors vector. At each iteration the algorithm determines the slowest node
601 according to the equation (\ref{eq:perf}) and keeps its frequency unchanged,
602 while it lowers the frequency of all other nodes by one gear. The new overall
603 energy consumption and execution time are computed according to the new scaling
604 factors. The optimal set of frequency scaling factors is the set that gives the
605 highest distance according to the objective function (\ref{eq:max}).
607 Figures~\ref{fig:r1} and \ref{fig:r2} illustrate the normalized performance and
608 consumed energy for an application running on a homogeneous platform and a
609 heterogeneous platform respectively while increasing the scaling factors. It can
610 be noticed that in a homogeneous platform the search for the optimal scaling
611 factor should start from the maximum frequency because the performance and the
612 consumed energy decrease from the beginning of the plot. On the other hand,
613 in the heterogeneous platform the performance is maintained at the beginning of
614 the plot even if the frequencies of the faster nodes decrease until the
615 computing power of scaled down nodes are lower than the slowest node. In other
616 words, until they reach the higher bound. It can also be noticed that the higher
617 the difference between the faster nodes and the slower nodes is, the bigger the
618 maximum distance between the energy curve and the performance curve is while
619 the scaling factors are varying which results in bigger energy savings.
622 \includegraphics[scale=0.5]{fig/start_freq}
623 \caption{Selecting the initial frequencies}
631 \begin{algorithmic}[1]
635 \item[$\Tcp_i$] array of all computation times for all nodes during one iteration and with highest frequency.
636 \item[$\Tcm_i$] array of all communication times for all nodes during one iteration and with highest frequency.
637 \item[$\Fmax_i$] array of the maximum frequencies for all nodes.
638 \item[$\Pd_i$] array of the dynamic powers for all nodes.
639 \item[$\Ps_i$] array of the static powers for all nodes.
640 \item[$\Fdiff_i$] array of the difference between two successive frequencies for all nodes.
642 \Ensure $\Sopt_1,\Sopt_2 \dots, \Sopt_N$ is a vector of optimal scaling factors
644 \State $\Scp_i \gets \frac{\max_{i=1,2,\dots,N}(\Tcp_i)}{\Tcp_i} $
645 \State $F_{i} \gets \frac{\Fmax_i}{\Scp_i},~{i=1,2,\cdots,N}$
646 \State Round the computed initial frequencies $F_i$ to the closest one available in each node.
647 \If{(not the first frequency)}
648 \State $F_i \gets F_i+\Fdiff_i,~i=1,\dots,N.$
650 \State $\Told \gets max_{~i=1,\dots,N } (\Tcp_i+\Tcm_i)$
651 % \State $\Eoriginal \gets \sum_{i=1}^{N}{( \Pd_i \cdot \Tcp_i)} +\sum_{i=1}^{N} {(\Ps_i \cdot \Told)}$
652 \State $\Eoriginal \gets \sum_{i=1}^{N}{( \Pd_i \cdot \Tcp_i + \Ps_i \cdot \Told)}$
653 \State $\Sopt_{i} \gets 1,~i=1,\dots,N. $
654 \State $\Dist \gets 0 $
655 \While {(all nodes not reach their minimum frequency)}
656 \If{(not the last freq. \textbf{and} not the slowest node)}
657 \State $F_i \gets F_i - \Fdiff_i,~i=1,\dots,N.$
658 \State $S_i \gets \frac{\Fmax_i}{F_i},~i=1,\dots,N.$
660 \State $\Tnew \gets max_\textit{~i=1,\dots,N} (\Tcp_{i} \cdot S_{i}) + \MinTcm $
661 % \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)}} $
662 \State $\Ereduced \gets \sum_{i=1}^{N}{(S_i^{-2} \cdot \Pd_i \cdot \Tcp_i + \Ps_i \cdot \rlap{\Tnew)}} $
663 \State $\Pnorm \gets \frac{\Told}{\Tnew}$
664 \State $\Enorm\gets \frac{\Ereduced}{\Eoriginal}$
665 \If{$(\Pnorm - \Enorm > \Dist)$}
666 \State $\Sopt_{i} \gets S_{i},~i=1,\dots,N. $
667 \State $\Dist \gets \Pnorm - \Enorm$
670 \State Return $\Sopt_1,\Sopt_2,\dots,\Sopt_N$
672 \caption{frequency scaling factors selection algorithm}
677 \begin{algorithmic}[1]
679 \For {$k=1$ to \textit{some iterations}}
680 \State Computations section.
681 \State Communications section.
683 \State Gather all times of computation and\newline\hspace*{3em}%
684 communication from each node.
685 \State Call Algorithm \ref{HSA}.
686 \State Compute the new frequencies from the\newline\hspace*{3em}%
687 returned optimal scaling factors.
688 \State Set the new frequencies to nodes.
692 \caption{DVFS algorithm}
696 \subsection{The evaluation of the proposed algorithm}
697 \label{sec.verif.algo}
698 The precision of the proposed algorithm mainly depends on the execution time
699 prediction model defined in (\ref{eq:perf}) and the energy model computed by
700 (\ref{eq:energy}). The energy model is also significantly dependent on the
701 execution time model because the static energy is linearly related to the
702 execution time and the dynamic energy is related to the computation time. So,
703 all the works presented in this paper are based on the execution time model. To
704 verify this model, the predicted execution time was compared to the real
705 execution time over SimGrid/SMPI simulator,
706 v3.10~\cite{casanova+giersch+legrand+al.2014.versatile}, for all the NAS
707 parallel benchmarks NPB v3.3 \cite{NAS.Parallel.Benchmarks}, running class B on
708 8 or 9 nodes. The comparison showed that the proposed execution time model is
709 very precise, the maximum normalized difference between the predicted execution
710 time and the real execution time is equal to 0.03 for all the NAS benchmarks.
712 Since the proposed algorithm is not an exact method it does not test all the
713 possible solutions (vectors of scaling factors) in the search space. To prove
714 its efficiency, it was compared on small instances to a brute force search
715 algorithm that tests all the possible solutions. The brute force algorithm was
716 applied to different NAS benchmarks classes with different number of nodes. The
717 solutions returned by the brute force algorithm and the proposed algorithm were
718 identical and the proposed algorithm was on average 10 times faster than the
719 brute force algorithm. It has a small execution time: for a heterogeneous
720 cluster composed of four different types of nodes having the characteristics
721 presented in Table~\ref{table:platform}, it takes on average \np[ms]{0.04} for 4
722 nodes and \np[ms]{0.15} on average for 144 nodes to compute the best scaling
723 factors vector. The algorithm complexity is $O(F\cdot (N \cdot4) )$, where $F$
724 is the number of iterations and $N$ is the number of computing nodes. The
725 algorithm needs from 12 to 20 iterations to select the best vector of frequency
726 scaling factors that gives the results of the next sections.
728 \section{Experimental results}
730 To evaluate the efficiency and the overall energy consumption reduction of
731 Algorithm~\ref{HSA}, it was applied to the NAS parallel benchmarks NPB v3.3. The
732 experiments were executed on the simulator SimGrid/SMPI which offers easy tools
733 to create a heterogeneous platform and run message passing applications over it.
734 The heterogeneous platform that was used in the experiments, had one core per
735 node because just one process was executed per node. The heterogeneous platform
736 was composed of four types of nodes. Each type of nodes had different
737 characteristics such as the maximum CPU frequency, the number of available
738 frequencies and the computational power, see Table~\ref{table:platform}. The
739 characteristics of these different types of nodes are inspired from the
740 specifications of real Intel processors. The heterogeneous platform had up to
741 144 nodes and had nodes from the four types in equal proportions, for example if
742 a benchmark was executed on 8 nodes, 2 nodes from each type were used. Since the
743 constructors of CPUs do not specify the dynamic and the static power of their
744 CPUs, for each type of node they were chosen proportionally to its computing
745 power (FLOPS). In the initial heterogeneous platform, while computing with
746 highest frequency, each node consumed an amount of power proportional to its
747 computing power (which corresponds to 80\% of its dynamic power and the
748 remaining 20\% to the static power), the same assumption was made in
749 \cite{Our_first_paper,Rauber_Analytical.Modeling.for.Energy}. Finally, These
750 nodes were connected via an Ethernet network with 1 Gbit/s bandwidth.
754 \caption{Heterogeneous nodes characteristics}
757 \begin{tabular}{|*{7}{l|}}
759 Node &Simulated & Max & Min & Diff. & Dynamic & Static \\
760 type &GFLOPS & Freq. & Freq. & Freq. & power & power \\
761 & & GHz & GHz &GHz & & \\
763 1 &40 & 2.5 & 1.2 & 0.1 & 20~W &4~W \\
766 2 &50 & 2.66 & 1.6 & 0.133 & 25~W &5~W \\
769 3 &60 & 2.9 & 1.2 & 0.1 & 30~W &6~W \\
772 4 &70 & 3.4 & 1.6 & 0.133 & 35~W &7~W \\
776 \label{table:platform}
780 %\subsection{Performance prediction verification}
783 \subsection{The experimental results of the scaling algorithm}
787 The proposed algorithm was applied to the seven parallel NAS benchmarks (EP, CG,
788 MG, FT, BT, LU and SP) and the benchmarks were executed with the three classes:
789 A, B and C. However, due to the lack of space in this paper, only the results of
790 the biggest class, C, are presented while being run on different number of
791 nodes, ranging from 4 to 128 or 144 nodes depending on the benchmark being
792 executed. Indeed, the benchmarks CG, MG, LU, EP and FT had to be executed on $1,
793 2, 4, 8, 16, 32, 64, 128$ nodes. The other benchmarks such as BT and SP had to
794 be executed on $1, 4, 9, 16, 36, 64, 144$ nodes.
799 \caption{Running NAS benchmarks on 4 nodes }
802 \begin{tabular}{|*{7}{r|}}
805 Program & Execution & Energy & Energy & Performance & Distance \\
806 name & time/s & consumption/J & saving\% & degradation\% & \\
808 CG & 64.64 & 3560.39 &34.16 &6.72 &27.44 \\
810 MG & 18.89 & 1074.87 &35.37 &4.34 &31.03 \\
812 EP &79.73 &5521.04 &26.83 &3.04 &23.79 \\
814 LU &308.65 &21126.00 &34.00 &6.16 &27.84 \\
816 BT &360.12 &21505.55 &35.36 &8.49 &26.87 \\
818 SP &234.24 &13572.16 &35.22 &5.70 &29.52 \\
820 FT &81.58 &4151.48 &35.58 &0.99 &34.59 \\
828 \caption{Running NAS benchmarks on 8 and 9 nodes }
831 \begin{tabular}{|*{7}{r|}}
834 Program & Execution & Energy & Energy & Performance & Distance \\
835 name & time/s & consumption/J & saving\% & degradation\% & \\
837 CG &36.11 &3263.49 &31.25 &7.12 &24.13 \\
839 MG &8.99 &953.39 &33.78 &6.41 &27.37 \\
841 EP &40.39 &5652.81 &27.04 &0.49 &26.55 \\
843 LU &218.79 &36149.77 &28.23 &0.01 &28.22 \\
845 BT &166.89 &23207.42 &32.32 &7.89 &24.43 \\
847 SP &104.73 &18414.62 &24.73 &2.78 &21.95 \\
849 FT &51.10 &4913.26 &31.02 &2.54 &28.48 \\
857 \caption{Running NAS benchmarks on 16 nodes }
860 \begin{tabular}{|*{7}{r|}}
863 Program & Execution & Energy & Energy & Performance & Distance \\
864 name & time/s & consumption/J & saving\% & degradation\% & \\
866 CG &31.74 &4373.90 &26.29 &9.57 &16.72 \\
868 MG &5.71 &1076.19 &32.49 &6.05 &26.44 \\
870 EP &20.11 &5638.49 &26.85 &0.56 &26.29 \\
872 LU &144.13 &42529.06 &28.80 &6.56 &22.24 \\
874 BT &97.29 &22813.86 &34.95 &5.80 &29.15 \\
876 SP &66.49 &20821.67 &22.49 &3.82 &18.67 \\
878 FT &37.01 &5505.60 &31.59 &6.48 &25.11 \\
881 \label{table:res_16n}
886 \caption{Running NAS benchmarks on 32 and 36 nodes }
889 \begin{tabular}{|*{7}{r|}}
892 Program & Execution & Energy & Energy & Performance & Distance \\
893 name & time/s & consumption/J & saving\% & degradation\% & \\
895 CG &32.35 &6704.21 &16.15 &5.30 &10.85 \\
897 MG &4.30 &1355.58 &28.93 &8.85 &20.08 \\
899 EP &9.96 &5519.68 &26.98 &0.02 &26.96 \\
901 LU &99.93 &67463.43 &23.60 &2.45 &21.15 \\
903 BT &48.61 &23796.97 &34.62 &5.83 &28.79 \\
905 SP &46.01 &27007.43 &22.72 &3.45 &19.27 \\
907 FT &28.06 &7142.69 &23.09 &2.90 &20.19 \\
910 \label{table:res_32n}
915 \caption{Running NAS benchmarks on 64 nodes }
918 \begin{tabular}{|*{7}{r|}}
921 Program & Execution & Energy & Energy & Performance & Distance \\
922 name & time/s & consumption/J & saving\% & degradation\% & \\
924 CG &46.65 &17521.83 &8.13 &1.68 &6.45 \\
926 MG &3.27 &1534.70 &29.27 &14.35 &14.92 \\
928 EP &5.05 &5471.1084 &27.12 &3.11 &24.01 \\
930 LU &73.92 &101339.16 &21.96 &3.67 &18.29 \\
932 BT &39.99 &27166.71 &32.02 &12.28 &19.74 \\
934 SP &52.00 &49099.28 &24.84 &0.03 &24.81 \\
936 FT &25.97 &10416.82 &20.15 &4.87 &15.28 \\
939 \label{table:res_64n}
944 \caption{Running NAS benchmarks on 128 and 144 nodes }
947 \begin{tabular}{|*{7}{r|}}
950 Program & Execution & Energy & Energy & Performance & Distance \\
951 name & time/s & consumption/J & saving\% & degradation\% & \\
953 CG &56.92 &41163.36 &4.00 &1.10 &2.90 \\
955 MG &3.55 &2843.33 &18.77 &10.38 &8.39 \\
957 EP &2.67 &5669.66 &27.09 &0.03 &27.06 \\
959 LU &51.23 &144471.90 &16.67 &2.36 &14.31 \\
961 BT &37.96 &44243.82 &23.18 &1.28 &21.90 \\
963 SP &64.53 &115409.71 &26.72 &0.05 &26.67 \\
965 FT &25.51 &18808.72 &12.85 &2.84 &10.01 \\
968 \label{table:res_128n}
970 The overall energy consumption was computed for each instance according to the
971 energy consumption model (\ref{eq:energy}), with and without applying the
972 algorithm. The execution time was also measured for all these experiments. Then,
973 the energy saving and performance degradation percentages were computed for each
974 instance. The results are presented in Tables~\ref{table:res_4n},
975 \ref{table:res_8n}, \ref{table:res_16n}, \ref{table:res_32n},
976 \ref{table:res_64n} and \ref{table:res_128n}. All these results are the average
977 values from many experiments for energy savings and performance degradation.
978 The tables show the experimental results for running the NAS parallel benchmarks
979 on different number of nodes. The experiments show that the algorithm
980 significantly reduces the energy consumption (up to 35\%) and tries to limit the
981 performance degradation. They also show that the energy saving percentage
982 decreases when the number of computing nodes increases. This reduction is due
983 to the increase of the communication times compared to the execution times when
984 the benchmarks are run over a high number of nodes. Indeed, the benchmarks with
985 the same class, C, are executed on different numbers of nodes, so the
986 computation required for each iteration is divided by the number of computing
987 nodes. On the other hand, more communications are required when increasing the
988 number of nodes so the static energy increases linearly according to the
989 communication time and the dynamic power is less relevant in the overall energy
990 consumption. Therefore, reducing the frequency with Algorithm~\ref{HSA} is
991 less effective in reducing the overall energy savings. It can also be noticed
992 that for the benchmarks EP and SP that contain little or no communications, the
993 energy savings are not significantly affected by the high number of nodes. No
994 experiments were conducted using bigger classes than D, because they require a
995 lot of memory (more than 64GB) when being executed by the simulator on one
996 machine. The maximum distance between the normalized energy curve and the
997 normalized performance for each instance is also shown in the result tables. It
998 decrease in the same way as the energy saving percentage. The tables also show
999 that the performance degradation percentage is not significantly increased when
1000 the number of computing nodes is increased because the computation times are
1001 small when compared to the communication times.
1007 \subfloat[Energy saving]{%
1008 \includegraphics[width=.33\textwidth]{fig/energy}\label{fig:energy}}%
1010 \subfloat[Performance degradation ]{%
1011 \includegraphics[width=.33\textwidth]{fig/per_deg}\label{fig:per_deg}}
1013 \caption{The energy and performance for all NAS benchmarks running with a different number of nodes}
1016 Figures~\ref{fig:energy} and \ref{fig:per_deg} present the energy saving and
1017 performance degradation respectively for all the benchmarks according to the
1018 number of used nodes. As shown in the first plot, the energy saving percentages
1019 of the benchmarks MG, LU, BT and FT decrease linearly when the number of nodes
1020 increase. While for the EP and SP benchmarks, the energy saving percentage is
1021 not affected by the increase of the number of computing nodes, because in these
1022 benchmarks there are little or no communications. Finally, the energy saving of
1023 the GC benchmark significantly decrease when the number of nodes increase
1024 because this benchmark has more communications than the others. The second plot
1025 shows that the performance degradation percentages of most of the benchmarks
1026 decrease when they run on a big number of nodes because they spend more time
1027 communicating than computing, thus, scaling down the frequencies of some nodes
1028 has less effect on the performance.
1033 \subsection{The results for different power consumption scenarios}
1035 The results of the previous section were obtained while using processors that
1036 consume during computation an overall power which is 80\% composed of dynamic
1037 power and of 20\% of static power. In this section, these ratios are changed and
1038 two new power scenarios are considered in order to evaluate how the proposed
1039 algorithm adapts itself according to the static and dynamic power values. The
1040 two new power scenarios are the following:
1043 \item 70\% of dynamic power and 30\% of static power
1044 \item 90\% of dynamic power and 10\% of static power
1047 The NAS parallel benchmarks were executed again over processors that follow the
1048 new power scenarios. The class C of each benchmark was run over 8 or 9 nodes
1049 and the results are presented in Tables~\ref{table:res_s1} and
1050 \ref{table:res_s2}. These tables show that the energy saving percentage of the
1051 70\%-30\% scenario is smaller for all benchmarks compared to the energy saving
1052 of the 90\%-10\% scenario. Indeed, in the latter more dynamic power is consumed
1053 when nodes are running on their maximum frequencies, thus, scaling down the
1054 frequency of the nodes results in higher energy savings than in the 70\%-30\%
1055 scenario. On the other hand, the performance degradation percentage is smaller
1056 in the 70\%-30\% scenario compared to the 90\%-10\% scenario. This is due to the
1057 higher static power percentage in the first scenario which makes it more
1058 relevant in the overall consumed energy. Indeed, the static energy is related
1059 to the execution time and if the performance is degraded the amount of consumed
1060 static energy directly increases. Therefore, the proposed algorithm does not
1061 really significantly scale down much the frequencies of the nodes in order to
1062 limit the increase of the execution time and thus limiting the effect of the
1063 consumed static energy.
1065 Both new power scenarios are compared to the old one in
1066 Figure~\ref{fig:sen_comp}. It shows the average of the performance degradation, the
1067 energy saving and the distances for all NAS benchmarks of class C running on 8
1068 or 9 nodes. The comparison shows that the energy saving ratio is proportional
1069 to the dynamic power ratio: it is increased when applying the 90\%-10\% scenario
1070 because at maximum frequency the dynamic energy is the most relevant in the
1071 overall consumed energy and can be reduced by lowering the frequency of some
1072 processors. On the other hand, the energy saving decreases when the 70\%-30\%
1073 scenario is used because the dynamic energy is less relevant in the overall
1074 consumed energy and lowering the frequency does not return big energy savings.
1075 Moreover, the average of the performance degradation is decreased when using a
1076 higher ratio for static power (e.g. 70\%-30\% scenario and 80\%-20\%
1077 scenario). Since the proposed algorithm optimizes the energy consumption when
1078 using a higher ratio for dynamic power the algorithm selects bigger frequency
1079 scaling factors that result in more energy saving but less performance, for
1080 example see Figure~\ref{fig:scales_comp}. The opposite happens when using a
1081 higher ratio for static power, the algorithm proportionally selects smaller
1082 scaling values which result in less energy saving but also less performance
1087 \caption{The results of the 70\%-30\% power scenario}
1090 \begin{tabular}{|*{6}{r|}}
1092 Program & Energy & Energy & Performance & Distance \\
1093 name & consumption/J & saving\% & degradation\% & \\
1095 CG &4144.21 &22.42 &7.72 &14.70 \\
1097 MG &1133.23 &24.50 &5.34 &19.16 \\
1099 EP &6170.30 &16.19 &0.02 &16.17 \\
1101 LU &39477.28 &20.43 &0.07 &20.36 \\
1103 BT &26169.55 &25.34 &6.62 &18.71 \\
1105 SP &19620.09 &19.32 &3.66 &15.66 \\
1107 FT &6094.07 &23.17 &0.36 &22.81 \\
1110 \label{table:res_s1}
1116 \caption{The results of the 90\%-10\% power scenario}
1119 \begin{tabular}{|*{6}{r|}}
1121 Program & Energy & Energy & Performance & Distance \\
1122 name & consumption/J & saving\% & degradation\% & \\
1124 CG &2812.38 &36.36 &6.80 &29.56 \\
1126 MG &825.427 &38.35 &6.41 &31.94 \\
1128 EP &5281.62 &35.02 &2.68 &32.34 \\
1130 LU &31611.28 &39.15 &3.51 &35.64 \\
1132 BT &21296.46 &36.70 &6.60 &30.10 \\
1134 SP &15183.42 &35.19 &11.76 &23.43 \\
1136 FT &3856.54 &40.80 &5.67 &35.13 \\
1139 \label{table:res_s2}
1145 \subfloat[Comparison between the results on 8 nodes]{%
1146 \includegraphics[width=.33\textwidth]{fig/sen_comp}\label{fig:sen_comp}}%
1148 \subfloat[Comparison the selected frequency scaling factors of MG benchmark class C running on 8 nodes]{%
1149 \includegraphics[width=.33\textwidth]{fig/three_scenarios}\label{fig:scales_comp}}
1151 \caption{The comparison of the three power scenarios}
1157 \subsection{The comparison of the proposed scaling algorithm }
1158 \label{sec.compare_EDP}
1159 In this section, the scaling factors selection algorithm, called $\MaxDist$,
1160 is compared to Spiliopoulos et al. algorithm \cite{Spiliopoulos_Green.governors.Adaptive.DVFS}, called EDP.
1161 They developed a green governor that regularly applies an online frequency selecting algorithm to reduce the energy consumed by a multicore architecture without degrading much its performance. The algorithm selects the frequencies that minimize the energy and delay products, $EDP=Energy\cdot Delay$ using the predicted overall energy consumption and execution time delay for each frequency.
1162 To fairly compare both algorithms, the same energy and execution time models, equations (\ref{eq:energy}) and (\ref{eq:fnew}), were used for both algorithms to predict the energy consumption and the execution times. Also Spiliopoulos et al. algorithm was adapted to start the search from the
1163 initial frequencies computed using the equation (\ref{eq:Fint}). The resulting algorithm is an exhaustive search algorithm that minimizes the EDP and has the initial frequencies values as an upper bound.
1165 Both algorithms were applied to the parallel NAS benchmarks to compare their
1166 efficiency. Table~\ref{table:compare_EDP} presents the results of comparing the
1167 execution times and the energy consumption for both versions of the NAS
1168 benchmarks while running the class C of each benchmark over 8 or 9 heterogeneous
1169 nodes. The results show that our algorithm provides better energy savings than
1170 Spiliopoulos et al. algorithm, on average it results in 29.76\% energy saving
1171 while their algorithm returns just 25.75\%. The average of performance
1172 degradation percentage is approximately the same for both algorithms, about 4\%.
1175 For all benchmarks, our algorithm outperforms Spiliopoulos et al. algorithm in
1176 terms of energy and performance trade-off, see Figure~\ref{fig:compare_EDP},
1177 because it maximizes the distance between the energy saving and the performance
1178 degradation values while giving the same weight for both metrics.
1184 \caption{Comparing the proposed algorithm}
1186 \begin{tabular}{|*{7}{r|}}
1188 Program & \multicolumn{2}{c|}{Energy saving \%} & \multicolumn{2}{c|}{Perf. degradation \%} & \multicolumn{2}{c|}{Distance} \\ \cline{2-7}
1189 name & EDP & MaxDist & EDP & MaxDist & EDP & MaxDist \\ \hline
1190 CG & 27.58 & 31.25 & 5.82 & 7.12 & 21.76 & 24.13 \\ \hline
1191 MG & 29.49 & 33.78 & 3.74 & 6.41 & 25.75 & 27.37 \\ \hline
1192 LU & 19.55 & 28.33 & 0.0 & 0.01 & 19.55 & 28.22 \\ \hline
1193 EP & 28.40 & 27.04 & 4.29 & 0.49 & 24.11 & 26.55 \\ \hline
1194 BT & 27.68 & 32.32 & 6.45 & 7.87 & 21.23 & 24.43 \\ \hline
1195 SP & 20.52 & 24.73 & 5.21 & 2.78 & 15.31 & 21.95 \\ \hline
1196 FT & 27.03 & 31.02 & 2.75 & 2.54 & 24.28 & 28.48 \\ \hline
1199 \label{table:compare_EDP}
1208 \includegraphics[scale=0.5]{fig/compare_EDP.pdf}
1209 \caption{Trade-off comparison for NAS benchmarks class C}
1210 \label{fig:compare_EDP}
1214 \section{Conclusion}
1216 In this paper, a new online frequency selecting algorithm has been presented. It
1217 selects the best possible vector of frequency scaling factors that gives the
1218 maximum distance (optimal trade-off) between the predicted energy and the
1219 predicted performance curves for a heterogeneous platform. This algorithm uses a
1220 new energy model for measuring and predicting the energy of distributed
1221 iterative applications running over heterogeneous platforms. To evaluate the
1222 proposed method, it was applied on the NAS parallel benchmarks and executed over
1223 a heterogeneous platform simulated by SimGrid. The results of the experiments
1224 showed that the algorithm reduces up to 35\% the energy consumption of a message
1225 passing iterative method while limiting the degradation of the performance. The
1226 algorithm also selects different scaling factors according to the percentage of
1227 the computing and communication times, and according to the values of the static
1228 and dynamic powers of the CPUs. Finally, the algorithm was compared to
1229 Spiliopoulos et al. algorithm and the results showed that it outperforms their
1230 algorithm in terms of energy-time trade-off.
1232 In the near future, this method will be applied to real heterogeneous platforms
1233 to evaluate its performance in a real study case. It would also be interesting
1234 to evaluate its scalability over large scale heterogeneous platforms and measure
1235 the energy consumption reduction it can produce. Afterward, we would like to
1236 develop a similar method that is adapted to asynchronous iterative applications
1237 where each task does not wait for other tasks to finish their works. The
1238 development of such a method might require a new energy model because the number
1239 of iterations is not known in advance and depends on the global convergence of
1240 the iterative system.
1242 \section*{Acknowledgment}
1244 This work has been partially supported by the Labex
1245 ACTION project (contract “ANR-11-LABX-01-01”). As a PhD student,
1246 Mr. Ahmed Fanfakh, would like to thank the University of
1247 Babylon (Iraq) for supporting his work.
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