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59 \title{Energy Consumption Reduction for Message Passing Iterative Applications in Heterogeneous Architecture Using DVFS}
69 FEMTO-ST Institute, University of Franche-Comte\\
70 IUT de Belfort-Montbéliard,
71 19 avenue du Maréchal Juin, BP 527, 90016 Belfort cedex, France\\
72 % Telephone: \mbox{+33 3 84 58 77 86}, % Raphaël
73 % Fax: \mbox{+33 3 84 58 77 81}\\ % Dept Info
74 Email: \email{{jean-claude.charr,raphael.couturier,ahmed.fanfakh_badri_muslim,arnaud.giersch}@univ-fcomte.fr}
81 Computing platforms are consuming more and more energy due to the increasing
82 number of nodes composing them. To minimize the operating costs of these
83 platforms many techniques have been used. Dynamic voltage and frequency scaling
84 (DVFS) is one of them. It reduces the frequency of a CPU to lower its energy
85 consumption. However, lowering the frequency of a CPU might increase the
86 execution time of an application running on that processor. Therefore, the
87 frequency that gives the best trade-off between the energy consumption and the
88 performance of an application must be selected.\\
89 In this paper, a new online frequencies selecting algorithm for heterogeneous
90 platforms is presented. It selects the frequency which tries to give the best
91 trade-off between energy saving and performance degradation, for each node
92 computing the message passing iterative application. The algorithm has a small
93 overhead and works without training or profiling. It uses a new energy model for
94 message passing iterative applications running on a heterogeneous platform. The
95 proposed algorithm is evaluated on the SimGrid simulator while running the NAS
96 parallel benchmarks. The experiments show that it reduces the energy
97 consumption by up to 35\% while limiting the performance degradation as much as
98 possible. Finally, the algorithm is compared to an existing method, the
99 comparison results showing that it outperforms the latter.
103 \section{Introduction}
105 The need for more computing power is continually increasing. To partially
106 satisfy this need, most supercomputers constructors just put more computing
107 nodes in their platform. The resulting platforms might achieve higher floating
108 point operations per second (FLOPS), but the energy consumption and the heat
109 dissipation are also increased. As an example, the Chinese supercomputer
110 Tianhe-2 had the highest FLOPS in November 2014 according to the Top500 list
111 \cite{TOP500_Supercomputers_Sites}. However, it was also the most power hungry
112 platform with its over 3 million cores consuming around 17.8 megawatts.
113 Moreover, according to the U.S. annual energy outlook 2014
114 \cite{U.S_Annual.Energy.Outlook.2014}, the price of energy for 1 megawatt-hour
115 was approximately equal to \$70. Therefore, the price of the energy consumed by
116 the Tianhe-2 platform is approximately more than \$10 million each year. The
117 computing platforms must be more energy efficient and offer the highest number
118 of FLOPS per watt possible, such as the L-CSC from the GSI Helmholtz Center
119 which became the top of the Green500 list in November 2014 \cite{Green500_List}.
120 This heterogeneous platform executes more than 5 GFLOPS per watt while consuming
123 Besides platform improvements, there are many software and hardware techniques
124 to lower the energy consumption of these platforms, such as scheduling, DVFS,
125 \dots{} DVFS is a widely used process to reduce the energy consumption of a
126 processor by lowering its frequency
127 \cite{Rizvandi_Some.Observations.on.Optimal.Frequency}. However, it also reduces
128 the number of FLOPS executed by the processor which might increase the execution
129 time of the application running over that processor. Therefore, researchers use
130 different optimization strategies to select the frequency that gives the best
131 trade-off between the energy reduction and performance degradation ratio. In
132 \cite{Our_first_paper}, a frequency selecting algorithm was proposed to reduce
133 the energy consumption of message passing iterative applications running over
134 homogeneous platforms. The results of the experiments show significant energy
135 consumption reductions. In this paper, a new frequency selecting algorithm
136 adapted for heterogeneous platform is presented. It selects the vector of
137 frequencies, for a heterogeneous platform running a message passing iterative
138 application, that simultaneously tries to offer the maximum energy reduction and
139 minimum performance degradation ratio. The algorithm has a very small overhead,
140 works online and does not need any training or profiling.
142 This paper is organized as follows: Section~\ref{sec.relwork} presents some
143 related works from other authors. Section~\ref{sec.exe} describes how the
144 execution time of message passing programs can be predicted. It also presents an energy
145 model that predicts the energy consumption of an application running over a heterogeneous platform. Section~\ref{sec.compet} presents
146 the energy-performance objective function that maximizes the reduction of energy
147 consumption while minimizing the degradation of the program's performance.
148 Section~\ref{sec.optim} details the proposed frequency selecting algorithm then the precision of the proposed algorithm is verified.
149 Section~\ref{sec.expe} presents the results of applying the algorithm on the NAS parallel benchmarks and executing them
150 on a heterogeneous platform. It shows the results of running three
151 different power scenarios and comparing them. Moreover, it also shows the comparison results
152 between the proposed method and an existing method.
153 Finally, in Section~\ref{sec.concl} the paper ends with a summary and some future works.
155 \section{Related works}
157 DVFS is a technique used in modern processors to scale down both the voltage and
158 the frequency of the CPU while computing, in order to reduce the energy
159 consumption of the processor. DVFS is also allowed in GPUs to achieve the same
160 goal. Reducing the frequency of a processor lowers its number of FLOPS and might
161 degrade the performance of the application running on that processor, especially
162 if it is compute bound. Therefore selecting the appropriate frequency for a
163 processor to satisfy some objectives while taking into account all the
164 constraints, is not a trivial operation. Many researchers used different
165 strategies to tackle this problem. Some of them developed online methods that
166 compute the new frequency while executing the application, such
167 as~\cite{Hao_Learning.based.DVFS,Spiliopoulos_Green.governors.Adaptive.DVFS}.
168 Others used offline methods that might need to run the application and profile
169 it before selecting the new frequency, such
170 as~\cite{Rountree_Bounding.energy.consumption.in.MPI,Cochran_Pack_and_Cap_Adaptive_DVFS}.
171 The methods could be heuristics, exact or brute force methods that satisfy
172 varied objectives such as energy reduction or performance. They also could be
173 adapted to the execution's environment and the type of the application such as
174 sequential, parallel or distributed architecture, homogeneous or heterogeneous
175 platform, synchronous or asynchronous application, \dots{}
177 In this paper, we are interested in reducing energy for message passing iterative synchronous applications running over heterogeneous platforms.
178 Some works have already been done for such platforms and they can be classified into two types of heterogeneous platforms:
181 \item the platform is composed of homogeneous GPUs and homogeneous CPUs.
182 \item the platform is only composed of heterogeneous CPUs.
186 For the first type of platform, the computing intensive parallel tasks are
187 executed on the GPUs and the rest are executed on the CPUs. Luley et
188 al.~\cite{Luley_Energy.efficiency.evaluation.and.benchmarking}, proposed a
189 heterogeneous cluster composed of Intel Xeon CPUs and NVIDIA GPUs. Their main
190 goal was to maximize the energy efficiency of the platform during computation by
191 maximizing the number of FLOPS per watt generated.
192 In~\cite{KaiMa_Holistic.Approach.to.Energy.Efficiency.in.GPU-CPU}, Kai Ma et
193 al. developed a scheduling algorithm that distributes workloads proportional to
194 the computing power of the nodes which could be a GPU or a CPU. All the tasks
195 must be completed at the same time. In~\cite{Rong_Effects.of.DVFS.on.K20.GPU},
196 Rong et al. showed that a heterogeneous (GPUs and CPUs) cluster that enables
197 DVFS gave better energy and performance efficiency than other clusters only
200 The work presented in this paper concerns the second type of platform, with
201 heterogeneous CPUs. Many methods were conceived to reduce the energy
202 consumption of this type of platform. Naveen et
203 al.~\cite{Naveen_Power.Efficient.Resource.Scaling} developed a method that
204 minimizes the value of $\mathit{energy}\times \mathit{delay}^2$ (the delay is
205 the sum of slack times that happen during synchronous communications) by
206 dynamically assigning new frequencies to the CPUs of the heterogeneous
207 cluster. Lizhe et al.~\cite{Lizhe_Energy.aware.parallel.task.scheduling}
208 proposed an algorithm that divides the executed tasks into two types: the
209 critical and non critical tasks. The algorithm scales down the frequency of non
210 critical tasks proportionally to their slack and communication times while
211 limiting the performance degradation percentage to less than
212 10\%. In~\cite{Joshi_Blackbox.prediction.of.impact.of.DVFS}, they developed a
213 heterogeneous cluster composed of two types of Intel and AMD processors. They
214 use a gradient method to predict the impact of DVFS operations on performance.
215 In~\cite{Shelepov_Scheduling.on.Heterogeneous.Multicore} and
216 \cite{Li_Minimizing.Energy.Consumption.for.Frame.Based.Tasks}, the best
217 frequencies for a specified heterogeneous cluster are selected offline using
218 some heuristic. Chen et
219 al.~\cite{Chen_DVFS.under.quality.of.service.requirements} used a greedy dynamic
220 programming approach to minimize the power consumption of heterogeneous servers
221 while respecting given time constraints. This approach had considerable
222 overhead. In contrast to the above described papers, this paper presents the
223 following contributions :
225 \item two new energy and performance models for message passing iterative synchronous applications running over
226 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.
228 \item a new online frequency selecting algorithm for heterogeneous platforms. The algorithm has a very small
229 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.
233 \section{The performance and energy consumption measurements on heterogeneous architecture}
238 \subsection{The execution time of message passing distributed
239 iterative applications on a heterogeneous platform}
241 In this paper, we are interested in reducing the energy consumption of message
242 passing distributed iterative synchronous applications running over
243 heterogeneous platforms. A heterogeneous platform is defined as a collection of
244 heterogeneous computing nodes interconnected via a high speed homogeneous
245 network. Therefore, each node has different characteristics such as computing
246 power (FLOPS), energy consumption, CPU's frequency range, \dots{} but they all
247 have the same network bandwidth and latency.
249 The overall execution time of a distributed iterative synchronous application
250 over a heterogeneous platform consists of the sum of the computation time and
251 the communication time for every iteration on a node. However, due to the
252 heterogeneous computation power of the computing nodes, slack times might occur
253 when fast nodes have to wait, during synchronous communications, for the slower
254 nodes to finish their computations (see Figure~\ref{fig:heter}). Therefore, the
255 overall execution time of the program is the execution time of the slowest task
256 which has the highest computation time and no slack time.
260 \includegraphics[scale=0.6]{fig/commtasks}
261 \caption{Parallel tasks on a heterogeneous platform}
265 Dynamic Voltage and Frequency Scaling (DVFS) is a process, implemented in
266 modern processors, that reduces the energy consumption of a CPU by scaling
267 down its voltage and frequency. Since DVFS lowers the frequency of a CPU
268 and consequently its computing power, the execution time of a program running
269 over that scaled down processor might increase, especially if the program is
270 compute bound. The frequency reduction process can be expressed by the scaling
271 factor S which is the ratio between the maximum and the new frequency of a CPU
275 S = \frac{\Fmax}{\Fnew}
277 The execution time of a compute bound sequential program is linearly proportional
278 to the frequency scaling factor $S$. On the other hand, message passing
279 distributed applications consist of two parts: computation and communication.
280 The execution time of the computation part is linearly proportional to the
281 frequency scaling factor $S$ but the communication time is not affected by the
282 scaling factor because the processors involved remain idle during the
283 communications~\cite{Freeh_Exploring.the.Energy.Time.Tradeoff}.
284 The communication time for a task is the summation of periods of
285 time that begin with an MPI call for sending or receiving a message
286 until the message is synchronously sent or received.
288 Since in a heterogeneous platform each node has different characteristics,
289 especially different frequency gears, when applying DVFS operations on these
290 nodes, they may get different scaling factors represented by a scaling vector:
291 $(S_1, S_2,\dots, S_N)$ where $S_i$ is the scaling factor of processor $i$. To
292 be able to predict the execution time of message passing synchronous iterative
293 applications running over a heterogeneous platform, for different vectors of
294 scaling factors, the communication time and the computation time for all the
295 tasks must be measured during the first iteration before applying any DVFS
296 operation. Then the execution time for one iteration of the application with any
297 vector of scaling factors can be predicted using (\ref{eq:perf}).
300 \Tnew = \max_{i=1,2,\dots,N} ({\TcpOld_{i}} \cdot S_{i}) + \MinTcm
305 \MinTcm = \min_{i=1,2,\dots,N} (\Tcm_i)
307 where $\TcpOld_i$ is the computation time of processor $i$ during the first
308 iteration and $\MinTcm$ is the communication time of the slowest processor from
309 the first iteration. The model computes the maximum computation time with
310 scaling factor from each node added to the communication time of the slowest
311 node. It means only the communication time without any slack time is taken into
312 account. Therefore, the execution time of the iterative application is equal to
313 the execution time of one iteration as in (\ref{eq:perf}) multiplied by the
314 number of iterations of that application.
316 This prediction model is developed from the model to predict the execution time
317 of message passing distributed applications for homogeneous
318 architectures~\cite{Our_first_paper}. The execution time prediction model is
319 used in the method to optimize both the energy consumption and the performance of
320 iterative methods, which is presented in the following sections.
323 \subsection{Energy model for heterogeneous platform}
324 Many researchers~\cite{Malkowski_energy.efficient.high.performance.computing,
325 Rauber_Analytical.Modeling.for.Energy,Zhuo_Energy.efficient.Dynamic.Task.Scheduling,
326 Rizvandi_Some.Observations.on.Optimal.Frequency} divide the power consumed by a processor into
327 two power metrics: the static and the dynamic power. While the first one is
328 consumed as long as the computing unit is turned on, the latter is only consumed during
329 computation times. The dynamic power $\Pd$ is related to the switching
330 activity $\alpha$, load capacitance $\CL$, the supply voltage $V$ and
331 operational frequency $F$, as shown in (\ref{eq:pd}).
334 \Pd = \alpha \cdot \CL \cdot V^2 \cdot F
336 The static power $\Ps$ captures the leakage power as follows:
339 \Ps = V \cdot \Ntrans \cdot \Kdesign \cdot \Ileak
341 where V is the supply voltage, $\Ntrans$ is the number of transistors,
342 $\Kdesign$ is a design dependent parameter and $\Ileak$ is a
343 technology dependent parameter. The energy consumed by an individual processor
344 to execute a given program can be computed as:
347 \Eind = \Pd \cdot \Tcp + \Ps \cdot T
349 where $T$ is the execution time of the program, $\Tcp$ is the computation
350 time and $\Tcp \le T$. $\Tcp$ may be equal to $T$ if there is no
351 communication and no slack time.
353 The main objective of DVFS operation is to reduce the overall energy consumption~\cite{Le_DVFS.Laws.of.Diminishing.Returns}.
354 The operational frequency $F$ depends linearly on the supply voltage $V$, i.e., $V = \beta \cdot F$ with some
355 constant $\beta$.~This equation is used to study the change of the dynamic
356 voltage with respect to various frequency values in~\cite{Rauber_Analytical.Modeling.for.Energy}. The reduction
357 process of the frequency can be expressed by the scaling factor $S$ which is the
358 ratio between the maximum and the new frequency as in (\ref{eq:s}).
359 The CPU governors are power schemes supplied by the operating
360 system's kernel to lower a core's frequency. The new frequency
361 $\Fnew$ from (\ref{eq:s}) can be calculated as follows:
364 \Fnew = S^{-1} \cdot \Fmax
366 Replacing $\Fnew$ in (\ref{eq:pd}) as in (\ref{eq:fnew}) gives the following
367 equation for dynamic power consumption:
370 \PdNew = \alpha \cdot \CL \cdot V^2 \cdot \Fnew = \alpha \cdot \CL \cdot \beta^2 \cdot \Fnew^3 \\
371 {} = \alpha \cdot \CL \cdot V^2 \cdot \Fmax \cdot S^{-3} = \PdOld \cdot S^{-3}
373 where $\PdNew$ and $\PdOld$ are the dynamic power consumed with the
374 new frequency and the maximum frequency respectively.
376 According to (\ref{eq:pdnew}) the dynamic power is reduced by a factor of $S^{-3}$ when
377 reducing the frequency by a factor of $S$~\cite{Rauber_Analytical.Modeling.for.Energy}. Since the FLOPS of a CPU is proportional
378 to the frequency of a CPU, the computation time is increased proportionally to $S$.
379 The new dynamic energy is the dynamic power multiplied by the new time of computation
380 and is given by the following equation:
383 \EdNew = \PdOld \cdot S^{-3} \cdot (\Tcp \cdot S)= S^{-2}\cdot \PdOld \cdot \Tcp
385 The static power is related to the power leakage of the CPU and is consumed during computation
386 and even when idle. As in~\cite{Rauber_Analytical.Modeling.for.Energy,Zhuo_Energy.efficient.Dynamic.Task.Scheduling},
387 the static power of a processor is considered as constant
388 during idle and computation periods, and for all its available frequencies.
389 The static energy is the static power multiplied by the execution time of the program.
390 According to the execution time model in (\ref{eq:perf}), the execution time of the program
391 is the sum of the computation and the communication times. The computation time is linearly related
392 to the frequency scaling factor, while this scaling factor does not affect the communication time.
393 The static energy of a processor after scaling its frequency is computed as follows:
396 \Es = \Ps \cdot (\Tcp \cdot S + \Tcm)
399 In the considered heterogeneous platform, each processor $i$ might have
400 different dynamic and static powers, noted as $\Pd_{i}$ and $\Ps_{i}$
401 respectively. Therefore, even if the distributed message passing iterative
402 application is load balanced, the computation time of each CPU $i$ noted
403 $\Tcp_{i}$ might be different and different frequency scaling factors might be
404 computed in order to decrease the overall energy consumption of the application
405 and reduce slack times. The communication time of a processor $i$ is noted as
406 $\Tcm_{i}$ and could contain slack times when communicating with slower
407 nodes, see Figure~\ref{fig:heter}. Therefore, all nodes do not have equal
408 communication times. While the dynamic energy is computed according to the
409 frequency scaling factor and the dynamic power of each node as in
410 (\ref{eq:Edyn}), the static energy is computed as the sum of the execution time
411 of one iteration multiplied by the static power of each processor. The overall
412 energy consumption of a message passing distributed application executed over a
413 heterogeneous platform during one iteration is the summation of all dynamic and
414 static energies for each processor. It is computed as follows:
417 E = \sum_{i=1}^{N} {(S_i^{-2} \cdot \Pd_{i} \cdot \Tcp_i)} + {} \\
418 \sum_{i=1}^{N} (\Ps_{i} \cdot (\max_{i=1,2,\dots,N} (\Tcp_i \cdot S_{i}) +
422 Reducing the frequencies of the processors according to the vector of
423 scaling factors $(S_1, S_2,\dots, S_N)$ may degrade the performance of the
424 application and thus, increase the static energy because the execution time is
425 increased~\cite{Kim_Leakage.Current.Moore.Law}. The overall energy consumption for the iterative
426 application can be measured by measuring the energy consumption for one iteration as in (\ref{eq:energy})
427 multiplied by the number of iterations of that application.
430 \section{Optimization of both energy consumption and performance}
433 Using the lowest frequency for each processor does not necessarily give the most
434 energy efficient execution of an application. Indeed, even though the dynamic
435 power is reduced while scaling down the frequency of a processor, its
436 computation power is proportionally decreased. Hence, the execution time might
437 be drastically increased and during that time, dynamic and static powers are
438 being consumed. Therefore, it might cancel any gains achieved by scaling down
439 the frequency of all nodes to the minimum and the overall energy consumption of
440 the application might not be the optimal one. It is not trivial to select the
441 appropriate frequency scaling factor for each processor while considering the
442 characteristics of each processor (computation power, range of frequencies,
443 dynamic and static powers) and the task executed (computation/communication
444 ratio). The aim being to reduce the overall energy consumption and to avoid
445 increasing significantly the execution time. In our previous
446 work~\cite{Our_first_paper}, we proposed a method that selects the optimal
447 frequency scaling factor for a homogeneous cluster executing a message passing
448 iterative synchronous application while giving the best trade-off between the
449 energy consumption and the performance for such applications. In this work we
450 are interested in heterogeneous clusters as described above. Due to the
451 heterogeneity of the processors, a vector of scaling factors should
452 be selected and it must give the best trade-off between energy consumption and
455 The relation between the energy consumption and the execution time for an
456 application is complex and nonlinear, Thus, unlike the relation between the
457 execution time and the scaling factor, the relation between the energy and the
458 frequency scaling factors is nonlinear, for more details refer
459 to~\cite{Freeh_Exploring.the.Energy.Time.Tradeoff}. Moreover, these relations
460 are not measured using the same metric. To solve this problem, the execution
461 time is normalized by computing the ratio between the new execution time (after
462 scaling down the frequencies of some processors) and the initial one (with
463 maximum frequency for all nodes) as follows:
466 \Pnorm = \frac{\Tnew}{\Told}\\
467 {} = \frac{ \max_{i=1,2,\dots,N} (\Tcp_{i} \cdot S_{i}) +\MinTcm}
468 {\max_{i=1,2,\dots,N}{(\Tcp_i+\Tcm_i)}}
472 In the same way, the energy is normalized by computing the ratio between the consumed energy
473 while scaling down the frequency and the consumed energy with maximum frequency for all nodes:
476 \Enorm = \frac{\Ereduced}{\Eoriginal} \\
477 {} = \frac{ \sum_{i=1}^{N}{(S_i^{-2} \cdot \Pd_i \cdot \Tcp_i)} +
478 \sum_{i=1}^{N} {(\Ps_i \cdot \Tnew)}}{\sum_{i=1}^{N}{( \Pd_i \cdot \Tcp_i)} +
479 \sum_{i=1}^{N} {(\Ps_i \cdot \Told)}}
481 Where $\Ereduced$ and $\Eoriginal$ are computed using (\ref{eq:energy}) and
482 $\Tnew$ and $\Told$ are computed as in (\ref{eq:pnorm}).
485 goal is to optimize the energy and execution time at the same time, the normalized
486 energy and execution time curves are not in the same direction. According
487 to the equations~(\ref{eq:pnorm}) and (\ref{eq:enorm}), the vector of frequency
488 scaling factors $S_1,S_2,\dots,S_N$ reduce both the energy and the execution
489 time simultaneously. But the main objective is to produce maximum energy
490 reduction with minimum execution time reduction.
492 This problem can be solved by making the optimization process for energy and
493 execution time following the same direction. Therefore, the equation of the
494 normalized execution time is inverted which gives the normalized performance equation, as follows:
497 \Pnorm = \frac{\Told}{\Tnew}\\
498 = \frac{\max_{i=1,2,\dots,N}{(\Tcp_i+\Tcm_i)}}
499 { \max_{i=1,2,\dots,N} (\Tcp_{i} \cdot S_{i}) + \MinTcm}
505 \subfloat[Homogeneous platform]{%
506 \includegraphics[width=.33\textwidth]{fig/homo}\label{fig:r1}}%
509 \subfloat[Heterogeneous platform]{%
510 \includegraphics[width=.33\textwidth]{fig/heter}\label{fig:r2}}
512 \caption{The energy and performance relation}
515 Then, the objective function can be modeled in order to find the maximum
516 distance between the energy curve (\ref{eq:enorm}) and the performance curve
517 (\ref{eq:pnorm_inv}) over all available sets of scaling factors. This
518 represents the minimum energy consumption with minimum execution time (maximum
519 performance) at the same time, see Figure~\ref{fig:r1} or
520 Figure~\ref{fig:r2}. Then the objective function has the following form:
524 \mathop{\max_{i=1,\dots F}}_{j=1,\dots,N}
525 (\overbrace{\Pnorm(S_{ij})}^{\text{Maximize}} -
526 \overbrace{\Enorm(S_{ij})}^{\text{Minimize}} )
528 where $N$ is the number of nodes and $F$ is the number of available frequencies for each node.
529 Then, the optimal set of scaling factors that satisfies (\ref{eq:max}) can be selected.
530 The objective function can work with any energy model or any power values for each node
531 (static and dynamic powers). However, the most important energy reduction gain can be achieved when
532 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}.
534 \section{The scaling factors selection algorithm for heterogeneous platforms }
537 \subsection{The algorithm details}
538 In this section, Algorithm~\ref{HSA} is presented. It selects the frequency
539 scaling factors vector that gives the best trade-off between minimizing the
540 energy consumption and maximizing the performance of a message passing
541 synchronous iterative application executed on a heterogeneous platform. It works
542 online during the execution time of the iterative message passing program. It
543 uses information gathered during the first iteration such as the computation
544 time and the communication time in one iteration for each node. The algorithm is
545 executed after the first iteration and returns a vector of optimal frequency
546 scaling factors that satisfies the objective function (\ref{eq:max}). The
547 program applies DVFS operations to change the frequencies of the CPUs according
548 to the computed scaling factors. This algorithm is called just once during the
549 execution of the program. Algorithm~\ref{dvfs} shows where and when the proposed
550 scaling algorithm is called in the iterative MPI program.
552 The nodes in a heterogeneous platform have different computing powers, thus
553 while executing message passing iterative synchronous applications, fast nodes
554 have to wait for the slower ones to finish their computations before being able
555 to synchronously communicate with them as in Figure~\ref{fig:heter}. These
556 periods are called idle or slack times. The algorithm takes into account this
557 problem and tries to reduce these slack times when selecting the frequency
558 scaling factors vector. At first, it selects initial frequency scaling factors
559 that increase the execution times of fast nodes and minimize the differences
560 between the computation times of fast and slow nodes. The value of the initial
561 frequency scaling factor for each node is inversely proportional to its
562 computation time that was gathered from the first iteration. These initial
563 frequency scaling factors are computed as a ratio between the computation time
564 of the slowest node and the computation time of the node $i$ as follows:
567 \Scp_{i} = \frac{\max_{i=1,2,\dots,N}(\Tcp_i)}{\Tcp_i}
569 Using the initial frequency scaling factors computed in (\ref{eq:Scp}), the algorithm computes
570 the initial frequencies for all nodes as a ratio between the maximum frequency of node $i$
571 and the computation scaling factor $\Scp_i$ as follows:
574 F_{i} = \frac{\Fmax_i}{\Scp_i},~{i=1,2,\dots,N}
576 If the computed initial frequency for a node is not available in the gears of
577 that node, it is replaced by the nearest available frequency. In
578 Figure~\ref{fig:st_freq}, the nodes are sorted by their computing power in
579 ascending order and the frequencies of the faster nodes are scaled down
580 according to the computed initial frequency scaling factors. The resulting new
581 frequencies are colored in blue in Figure~\ref{fig:st_freq}. This set of
582 frequencies can be considered as a higher bound for the search space of the
583 optimal vector of frequencies because selecting frequency scaling factors higher
584 than the higher bound will not improve the performance of the application and it
585 will increase its overall energy consumption. Therefore the algorithm that
586 selects the frequency scaling factors starts the search method from these
587 initial frequencies and takes a downward search direction toward lower
588 frequencies. The algorithm iterates on all left frequencies, from the higher
589 bound until all nodes reach their minimum frequencies, to compute their overall
590 energy consumption and performance, and select the optimal frequency scaling
591 factors vector. At each iteration the algorithm determines the slowest node
592 according to the equation (\ref{eq:perf}) and keeps its frequency unchanged,
593 while it lowers the frequency of all other nodes by one gear. The new overall
594 energy consumption and execution time are computed according to the new scaling
595 factors. The optimal set of frequency scaling factors is the set that gives the
596 highest distance according to the objective function (\ref{eq:max}).
598 Figures~\ref{fig:r1} and \ref{fig:r2} illustrate the normalized performance and
599 consumed energy for an application running on a homogeneous platform and a
600 heterogeneous platform respectively while increasing the scaling factors. It can
601 be noticed that in a homogeneous platform the search for the optimal scaling
602 factor should start from the maximum frequency because the performance and the
603 consumed energy decrease from the beginning of the plot. On the other hand,
604 in the heterogeneous platform the performance is maintained at the beginning of
605 the plot even if the frequencies of the faster nodes decrease until the
606 computing power of scaled down nodes are lower than the slowest node. In other
607 words, until they reach the higher bound. It can also be noticed that the higher
608 the difference between the faster nodes and the slower nodes is, the bigger the
609 maximum distance between the energy curve and the performance curve is while
610 the scaling factors are varying which results in bigger energy savings.
613 \includegraphics[scale=0.5]{fig/start_freq}
614 \caption{Selecting the initial frequencies}
622 \begin{algorithmic}[1]
626 \item[$\Tcp_i$] array of all computation times for all nodes during one iteration and with highest frequency.
627 \item[$\Tcm_i$] array of all communication times for all nodes during one iteration and with highest frequency.
628 \item[$\Fmax_i$] array of the maximum frequencies for all nodes.
629 \item[$\Pd_i$] array of the dynamic powers for all nodes.
630 \item[$\Ps_i$] array of the static powers for all nodes.
631 \item[$\Fdiff_i$] array of the difference between two successive frequencies for all nodes.
633 \Ensure $\Sopt_1,\Sopt_2 \dots, \Sopt_N$ is a vector of optimal scaling factors
635 \State $\Scp_i \gets \frac{\max_{i=1,2,\dots,N}(\Tcp_i)}{\Tcp_i} $
636 \State $F_{i} \gets \frac{\Fmax_i}{\Scp_i},~{i=1,2,\cdots,N}$
637 \State Round the computed initial frequencies $F_i$ to the closest one available in each node.
638 \If{(not the first frequency)}
639 \State $F_i \gets F_i+\Fdiff_i,~i=1,\dots,N.$
641 \State $\Told \gets max_{~i=1,\dots,N } (\Tcp_i+\Tcm_i)$
642 % \State $\Eoriginal \gets \sum_{i=1}^{N}{( \Pd_i \cdot \Tcp_i)} +\sum_{i=1}^{N} {(\Ps_i \cdot \Told)}$
643 \State $\Eoriginal \gets \sum_{i=1}^{N}{( \Pd_i \cdot \Tcp_i + \Ps_i \cdot \Told)}$
644 \State $\Sopt_{i} \gets 1,~i=1,\dots,N. $
645 \State $\Dist \gets 0 $
646 \While {(all nodes not reach their minimum frequency)}
647 \If{(not the last freq. \textbf{and} not the slowest node)}
648 \State $F_i \gets F_i - \Fdiff_i,~i=1,\dots,N.$
649 \State $S_i \gets \frac{\Fmax_i}{F_i},~i=1,\dots,N.$
651 \State $\Tnew \gets max_\textit{~i=1,\dots,N} (\Tcp_{i} \cdot S_{i}) + \MinTcm $
652 % \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)}} $
653 \State $\Ereduced \gets \sum_{i=1}^{N}{(S_i^{-2} \cdot \Pd_i \cdot \Tcp_i + \Ps_i \cdot \rlap{\Tnew)}} $
654 \State $\Pnorm \gets \frac{\Told}{\Tnew}$
655 \State $\Enorm\gets \frac{\Ereduced}{\Eoriginal}$
656 \If{$(\Pnorm - \Enorm > \Dist)$}
657 \State $\Sopt_{i} \gets S_{i},~i=1,\dots,N. $
658 \State $\Dist \gets \Pnorm - \Enorm$
661 \State Return $\Sopt_1,\Sopt_2,\dots,\Sopt_N$
663 \caption{frequency scaling factors selection algorithm}
668 \begin{algorithmic}[1]
670 \For {$k=1$ to \textit{some iterations}}
671 \State Computations section.
672 \State Communications section.
674 \State Gather all times of computation and\newline\hspace*{3em}%
675 communication from each node.
676 \State Call Algorithm \ref{HSA}.
677 \State Compute the new frequencies from the\newline\hspace*{3em}%
678 returned optimal scaling factors.
679 \State Set the new frequencies to nodes.
683 \caption{DVFS algorithm}
687 \subsection{The evaluation of the proposed algorithm}
688 \label{sec.verif.algo}
689 The precision of the proposed algorithm mainly depends on the execution time
690 prediction model defined in (\ref{eq:perf}) and the energy model computed by
691 (\ref{eq:energy}). The energy model is also significantly dependent on the
692 execution time model because the static energy is linearly related to the
693 execution time and the dynamic energy is related to the computation time. So,
694 all the works presented in this paper are based on the execution time model. To
695 verify this model, the predicted execution time was compared to the real
696 execution time over SimGrid/SMPI simulator,
697 v3.10~\cite{casanova+giersch+legrand+al.2014.versatile}, for all the NAS
698 parallel benchmarks NPB v3.3 \cite{NAS.Parallel.Benchmarks}, running class B on
699 8 or 9 nodes. The comparison showed that the proposed execution time model is
700 very precise, the maximum normalized difference between the predicted execution
701 time and the real execution time is equal to 0.03 for all the NAS benchmarks.
703 Since the proposed algorithm is not an exact method it does not test all the
704 possible solutions (vectors of scaling factors) in the search space. To prove
705 its efficiency, it was compared on small instances to a brute force search
706 algorithm that tests all the possible solutions. The brute force algorithm was
707 applied to different NAS benchmarks classes with different number of nodes. The
708 solutions returned by the brute force algorithm and the proposed algorithm were
709 identical and the proposed algorithm was on average 10 times faster than the
710 brute force algorithm. It has a small execution time: for a heterogeneous
711 cluster composed of four different types of nodes having the characteristics
712 presented in Table~\ref{table:platform}, it takes on average \np[ms]{0.04} for 4
713 nodes and \np[ms]{0.15} on average for 144 nodes to compute the best scaling
714 factors vector. The algorithm complexity is $O(F\cdot (N \cdot4) )$, where $F$
715 is the number of iterations and $N$ is the number of computing nodes. The
716 algorithm needs from 12 to 20 iterations to select the best vector of frequency
717 scaling factors that gives the results of the next sections.
719 \section{Experimental results}
721 To evaluate the efficiency and the overall energy consumption reduction of
722 Algorithm~\ref{HSA}, it was applied to the NAS parallel benchmarks NPB v3.3. The
723 experiments were executed on the simulator SimGrid/SMPI which offers easy tools
724 to create a heterogeneous platform and run message passing applications over it.
725 The heterogeneous platform that was used in the experiments, had one core per
726 node because just one process was executed per node. The heterogeneous platform
727 was composed of four types of nodes. Each type of nodes had different
728 characteristics such as the maximum CPU frequency, the number of available
729 frequencies and the computational power, see Table~\ref{table:platform}. The
730 characteristics of these different types of nodes are inspired from the
731 specifications of real Intel processors. The heterogeneous platform had up to
732 144 nodes and had nodes from the four types in equal proportions, for example if
733 a benchmark was executed on 8 nodes, 2 nodes from each type were used. Since the
734 constructors of CPUs do not specify the dynamic and the static power of their
735 CPUs, for each type of node they were chosen proportionally to its computing
736 power (FLOPS). In the initial heterogeneous platform, while computing with
737 highest frequency, each node consumed an amount of power proportional to its
738 computing power (which corresponds to 80\% of its dynamic power and the
739 remaining 20\% to the static power), the same assumption was made in
740 \cite{Our_first_paper,Rauber_Analytical.Modeling.for.Energy}. Finally, These
741 nodes were connected via an Ethernet network with 1 Gbit/s bandwidth.
745 \caption{Heterogeneous nodes characteristics}
748 \begin{tabular}{|*{7}{l|}}
750 Node &Simulated & Max & Min & Diff. & Dynamic & Static \\
751 type &GFLOPS & Freq. & Freq. & Freq. & power & power \\
752 & & GHz & GHz &GHz & & \\
754 1 &40 & 2.5 & 1.2 & 0.1 & 20~W &4~W \\
757 2 &50 & 2.66 & 1.6 & 0.133 & 25~W &5~W \\
760 3 &60 & 2.9 & 1.2 & 0.1 & 30~W &6~W \\
763 4 &70 & 3.4 & 1.6 & 0.133 & 35~W &7~W \\
767 \label{table:platform}
771 %\subsection{Performance prediction verification}
774 \subsection{The experimental results of the scaling algorithm}
778 The proposed algorithm was applied to the seven parallel NAS benchmarks (EP, CG,
779 MG, FT, BT, LU and SP) and the benchmarks were executed with the three classes:
780 A, B and C. However, due to the lack of space in this paper, only the results of
781 the biggest class, C, are presented while being run on different number of
782 nodes, ranging from 4 to 128 or 144 nodes depending on the benchmark being
783 executed. Indeed, the benchmarks CG, MG, LU, EP and FT had to be executed on $1,
784 2, 4, 8, 16, 32, 64, 128$ nodes. The other benchmarks such as BT and SP had to
785 be executed on $1, 4, 9, 16, 36, 64, 144$ nodes.
790 \caption{Running NAS benchmarks on 4 nodes }
793 \begin{tabular}{|*{7}{r|}}
796 Program & Execution & Energy & Energy & Performance & Distance \\
797 name & time/s & consumption/J & saving\% & degradation\% & \\
799 CG & 64.64 & 3560.39 &34.16 &6.72 &27.44 \\
801 MG & 18.89 & 1074.87 &35.37 &4.34 &31.03 \\
803 EP &79.73 &5521.04 &26.83 &3.04 &23.79 \\
805 LU &308.65 &21126.00 &34.00 &6.16 &27.84 \\
807 BT &360.12 &21505.55 &35.36 &8.49 &26.87 \\
809 SP &234.24 &13572.16 &35.22 &5.70 &29.52 \\
811 FT &81.58 &4151.48 &35.58 &0.99 &34.59 \\
819 \caption{Running NAS benchmarks on 8 and 9 nodes }
822 \begin{tabular}{|*{7}{r|}}
825 Program & Execution & Energy & Energy & Performance & Distance \\
826 name & time/s & consumption/J & saving\% & degradation\% & \\
828 CG &36.11 &3263.49 &31.25 &7.12 &24.13 \\
830 MG &8.99 &953.39 &33.78 &6.41 &27.37 \\
832 EP &40.39 &5652.81 &27.04 &0.49 &26.55 \\
834 LU &218.79 &36149.77 &28.23 &0.01 &28.22 \\
836 BT &166.89 &23207.42 &32.32 &7.89 &24.43 \\
838 SP &104.73 &18414.62 &24.73 &2.78 &21.95 \\
840 FT &51.10 &4913.26 &31.02 &2.54 &28.48 \\
848 \caption{Running NAS benchmarks on 16 nodes }
851 \begin{tabular}{|*{7}{r|}}
854 Program & Execution & Energy & Energy & Performance & Distance \\
855 name & time/s & consumption/J & saving\% & degradation\% & \\
857 CG &31.74 &4373.90 &26.29 &9.57 &16.72 \\
859 MG &5.71 &1076.19 &32.49 &6.05 &26.44 \\
861 EP &20.11 &5638.49 &26.85 &0.56 &26.29 \\
863 LU &144.13 &42529.06 &28.80 &6.56 &22.24 \\
865 BT &97.29 &22813.86 &34.95 &5.80 &29.15 \\
867 SP &66.49 &20821.67 &22.49 &3.82 &18.67 \\
869 FT &37.01 &5505.60 &31.59 &6.48 &25.11 \\
872 \label{table:res_16n}
877 \caption{Running NAS benchmarks on 32 and 36 nodes }
880 \begin{tabular}{|*{7}{r|}}
883 Program & Execution & Energy & Energy & Performance & Distance \\
884 name & time/s & consumption/J & saving\% & degradation\% & \\
886 CG &32.35 &6704.21 &16.15 &5.30 &10.85 \\
888 MG &4.30 &1355.58 &28.93 &8.85 &20.08 \\
890 EP &9.96 &5519.68 &26.98 &0.02 &26.96 \\
892 LU &99.93 &67463.43 &23.60 &2.45 &21.15 \\
894 BT &48.61 &23796.97 &34.62 &5.83 &28.79 \\
896 SP &46.01 &27007.43 &22.72 &3.45 &19.27 \\
898 FT &28.06 &7142.69 &23.09 &2.90 &20.19 \\
901 \label{table:res_32n}
906 \caption{Running NAS benchmarks on 64 nodes }
909 \begin{tabular}{|*{7}{r|}}
912 Program & Execution & Energy & Energy & Performance & Distance \\
913 name & time/s & consumption/J & saving\% & degradation\% & \\
915 CG &46.65 &17521.83 &8.13 &1.68 &6.45 \\
917 MG &3.27 &1534.70 &29.27 &14.35 &14.92 \\
919 EP &5.05 &5471.1084 &27.12 &3.11 &24.01 \\
921 LU &73.92 &101339.16 &21.96 &3.67 &18.29 \\
923 BT &39.99 &27166.71 &32.02 &12.28 &19.74 \\
925 SP &52.00 &49099.28 &24.84 &0.03 &24.81 \\
927 FT &25.97 &10416.82 &20.15 &4.87 &15.28 \\
930 \label{table:res_64n}
935 \caption{Running NAS benchmarks on 128 and 144 nodes }
938 \begin{tabular}{|*{7}{r|}}
941 Program & Execution & Energy & Energy & Performance & Distance \\
942 name & time/s & consumption/J & saving\% & degradation\% & \\
944 CG &56.92 &41163.36 &4.00 &1.10 &2.90 \\
946 MG &3.55 &2843.33 &18.77 &10.38 &8.39 \\
948 EP &2.67 &5669.66 &27.09 &0.03 &27.06 \\
950 LU &51.23 &144471.90 &16.67 &2.36 &14.31 \\
952 BT &37.96 &44243.82 &23.18 &1.28 &21.90 \\
954 SP &64.53 &115409.71 &26.72 &0.05 &26.67 \\
956 FT &25.51 &18808.72 &12.85 &2.84 &10.01 \\
959 \label{table:res_128n}
961 The overall energy consumption was computed for each instance according to the
962 energy consumption model (\ref{eq:energy}), with and without applying the
963 algorithm. The execution time was also measured for all these experiments. Then,
964 the energy saving and performance degradation percentages were computed for each
965 instance. The results are presented in Tables~\ref{table:res_4n},
966 \ref{table:res_8n}, \ref{table:res_16n}, \ref{table:res_32n},
967 \ref{table:res_64n} and \ref{table:res_128n}. All these results are the average
968 values from many experiments for energy savings and performance degradation.
969 The tables show the experimental results for running the NAS parallel benchmarks
970 on different number of nodes. The experiments show that the algorithm
971 significantly reduces the energy consumption (up to 35\%) and tries to limit the
972 performance degradation. They also show that the energy saving percentage
973 decreases when the number of computing nodes increases. This reduction is due
974 to the increase of the communication times compared to the execution times when
975 the benchmarks are run over a high number of nodes. Indeed, the benchmarks with
976 the same class, C, are executed on different numbers of nodes, so the
977 computation required for each iteration is divided by the number of computing
978 nodes. On the other hand, more communications are required when increasing the
979 number of nodes so the static energy increases linearly according to the
980 communication time and the dynamic power is less relevant in the overall energy
981 consumption. Therefore, reducing the frequency with Algorithm~\ref{HSA} is
982 less effective in reducing the overall energy savings. It can also be noticed
983 that for the benchmarks EP and SP that contain little or no communications, the
984 energy savings are not significantly affected by the high number of nodes. No
985 experiments were conducted using bigger classes than D, because they require a
986 lot of memory (more than 64GB) when being executed by the simulator on one
987 machine. The maximum distance between the normalized energy curve and the
988 normalized performance for each instance is also shown in the result tables. It
989 decrease in the same way as the energy saving percentage. The tables also show
990 that the performance degradation percentage is not significantly increased when
991 the number of computing nodes is increased because the computation times are
992 small when compared to the communication times.
998 \subfloat[Energy saving]{%
999 \includegraphics[width=.33\textwidth]{fig/energy}\label{fig:energy}}%
1001 \subfloat[Performance degradation ]{%
1002 \includegraphics[width=.33\textwidth]{fig/per_deg}\label{fig:per_deg}}
1004 \caption{The energy and performance for all NAS benchmarks running with a different number of nodes}
1007 Figures~\ref{fig:energy} and \ref{fig:per_deg} present the energy saving and
1008 performance degradation respectively for all the benchmarks according to the
1009 number of used nodes. As shown in the first plot, the energy saving percentages
1010 of the benchmarks MG, LU, BT and FT decrease linearly when the number of nodes
1011 increase. While for the EP and SP benchmarks, the energy saving percentage is
1012 not affected by the increase of the number of computing nodes, because in these
1013 benchmarks there are little or no communications. Finally, the energy saving of
1014 the GC benchmark significantly decrease when the number of nodes increase
1015 because this benchmark has more communications than the others. The second plot
1016 shows that the performance degradation percentages of most of the benchmarks
1017 decrease when they run on a big number of nodes because they spend more time
1018 communicating than computing, thus, scaling down the frequencies of some nodes
1019 has less effect on the performance.
1024 \subsection{The results for different power consumption scenarios}
1026 The results of the previous section were obtained while using processors that
1027 consume during computation an overall power which is 80\% composed of dynamic
1028 power and of 20\% of static power. In this section, these ratios are changed and
1029 two new power scenarios are considered in order to evaluate how the proposed
1030 algorithm adapts itself according to the static and dynamic power values. The
1031 two new power scenarios are the following:
1034 \item 70\% of dynamic power and 30\% of static power
1035 \item 90\% of dynamic power and 10\% of static power
1038 The NAS parallel benchmarks were executed again over processors that follow the
1039 new power scenarios. The class C of each benchmark was run over 8 or 9 nodes
1040 and the results are presented in Tables~\ref{table:res_s1} and
1041 \ref{table:res_s2}. These tables show that the energy saving percentage of the
1042 70\%-30\% scenario is smaller for all benchmarks compared to the energy saving
1043 of the 90\%-10\% scenario. Indeed, in the latter more dynamic power is consumed
1044 when nodes are running on their maximum frequencies, thus, scaling down the
1045 frequency of the nodes results in higher energy savings than in the 70\%-30\%
1046 scenario. On the other hand, the performance degradation percentage is smaller
1047 in the 70\%-30\% scenario compared to the 90\%-10\% scenario. This is due to the
1048 higher static power percentage in the first scenario which makes it more
1049 relevant in the overall consumed energy. Indeed, the static energy is related
1050 to the execution time and if the performance is degraded the amount of consumed
1051 static energy directly increases. Therefore, the proposed algorithm does not
1052 really significantly scale down much the frequencies of the nodes in order to
1053 limit the increase of the execution time and thus limiting the effect of the
1054 consumed static energy.
1056 Both new power scenarios are compared to the old one in
1057 Figure~\ref{fig:sen_comp}. It shows the average of the performance degradation, the
1058 energy saving and the distances for all NAS benchmarks of class C running on 8
1059 or 9 nodes. The comparison shows that the energy saving ratio is proportional
1060 to the dynamic power ratio: it is increased when applying the 90\%-10\% scenario
1061 because at maximum frequency the dynamic energy is the most relevant in the
1062 overall consumed energy and can be reduced by lowering the frequency of some
1063 processors. On the other hand, the energy saving decreases when the 70\%-30\%
1064 scenario is used because the dynamic energy is less relevant in the overall
1065 consumed energy and lowering the frequency does not return big energy savings.
1066 Moreover, the average of the performance degradation is decreased when using a
1067 higher ratio for static power (e.g. 70\%-30\% scenario and 80\%-20\%
1068 scenario). Since the proposed algorithm optimizes the energy consumption when
1069 using a higher ratio for dynamic power the algorithm selects bigger frequency
1070 scaling factors that result in more energy saving but less performance, for
1071 example see Figure~\ref{fig:scales_comp}. The opposite happens when using a
1072 higher ratio for static power, the algorithm proportionally selects smaller
1073 scaling values which result in less energy saving but also less performance
1078 \caption{The results of the 70\%-30\% power scenario}
1081 \begin{tabular}{|*{6}{r|}}
1083 Program & Energy & Energy & Performance & Distance \\
1084 name & consumption/J & saving\% & degradation\% & \\
1086 CG &4144.21 &22.42 &7.72 &14.70 \\
1088 MG &1133.23 &24.50 &5.34 &19.16 \\
1090 EP &6170.30 &16.19 &0.02 &16.17 \\
1092 LU &39477.28 &20.43 &0.07 &20.36 \\
1094 BT &26169.55 &25.34 &6.62 &18.71 \\
1096 SP &19620.09 &19.32 &3.66 &15.66 \\
1098 FT &6094.07 &23.17 &0.36 &22.81 \\
1101 \label{table:res_s1}
1107 \caption{The results of the 90\%-10\% power scenario}
1110 \begin{tabular}{|*{6}{r|}}
1112 Program & Energy & Energy & Performance & Distance \\
1113 name & consumption/J & saving\% & degradation\% & \\
1115 CG &2812.38 &36.36 &6.80 &29.56 \\
1117 MG &825.427 &38.35 &6.41 &31.94 \\
1119 EP &5281.62 &35.02 &2.68 &32.34 \\
1121 LU &31611.28 &39.15 &3.51 &35.64 \\
1123 BT &21296.46 &36.70 &6.60 &30.10 \\
1125 SP &15183.42 &35.19 &11.76 &23.43 \\
1127 FT &3856.54 &40.80 &5.67 &35.13 \\
1130 \label{table:res_s2}
1134 \caption{Comparing the proposed algorithm}
1136 \begin{tabular}{|*{7}{r|}}
1138 Program & \multicolumn{2}{c|}{Energy saving \%} & \multicolumn{2}{c|}{Perf. degradation \%} & \multicolumn{2}{c|}{Distance} \\ \cline{2-7}
1139 name & EDP & MaxDist & EDP & MaxDist & EDP & MaxDist \\ \hline
1140 CG & 27.58 & 31.25 & 5.82 & 7.12 & 21.76 & 24.13 \\ \hline
1141 MG & 29.49 & 33.78 & 3.74 & 6.41 & 25.75 & 27.37 \\ \hline
1142 LU & 19.55 & 28.33 & 0.0 & 0.01 & 19.55 & 28.22 \\ \hline
1143 EP & 28.40 & 27.04 & 4.29 & 0.49 & 24.11 & 26.55 \\ \hline
1144 BT & 27.68 & 32.32 & 6.45 & 7.87 & 21.23 & 24.43 \\ \hline
1145 SP & 20.52 & 24.73 & 5.21 & 2.78 & 15.31 & 21.95 \\ \hline
1146 FT & 27.03 & 31.02 & 2.75 & 2.54 & 24.28 & 28.48 \\ \hline
1149 \label{table:compare_EDP}
1154 \subfloat[Comparison between the results on 8 nodes]{%
1155 \includegraphics[width=.33\textwidth]{fig/sen_comp}\label{fig:sen_comp}}%
1157 \subfloat[Comparison the selected frequency scaling factors of MG benchmark class C running on 8 nodes]{%
1158 \includegraphics[width=.33\textwidth]{fig/three_scenarios}\label{fig:scales_comp}}
1160 \caption{The comparison of the three power scenarios}
1165 \includegraphics[scale=0.5]{fig/compare_EDP.pdf}
1166 \caption{Trade-off comparison for NAS benchmarks class C}
1167 \label{fig:compare_EDP}
1171 \subsection{The comparison of the proposed scaling algorithm }
1172 \label{sec.compare_EDP}
1173 In this section, the scaling factors selection algorithm, called MaxDist, is
1174 compared to Spiliopoulos et al. algorithm
1175 \cite{Spiliopoulos_Green.governors.Adaptive.DVFS}, called EDP. They developed a
1176 green governor that regularly applies an online frequency selecting algorithm to
1177 reduce the energy consumed by a multicore architecture without degrading much
1178 its performance. The algorithm selects the frequencies that minimize the energy
1179 and delay products, $\mathit{EDP}=\mathit{energy}\times \mathit{delay}$ using
1180 the predicted overall energy consumption and execution time delay for each
1181 frequency. To fairly compare both algorithms, the same energy and execution
1182 time models, equations (\ref{eq:energy}) and (\ref{eq:fnew}), were used for both
1183 algorithms to predict the energy consumption and the execution times. Also
1184 Spiliopoulos et al. algorithm was adapted to start the search from the initial
1185 frequencies computed using the equation (\ref{eq:Fint}). The resulting algorithm
1186 is an exhaustive search algorithm that minimizes the EDP and has the initial
1187 frequencies values as an upper bound.
1189 Both algorithms were applied to the parallel NAS benchmarks to compare their
1190 efficiency. Table~\ref{table:compare_EDP} presents the results of comparing the
1191 execution times and the energy consumption for both versions of the NAS
1192 benchmarks while running the class C of each benchmark over 8 or 9 heterogeneous
1193 nodes. The results show that our algorithm provides better energy savings than
1194 Spiliopoulos et al. algorithm, on average it results in 29.76\% energy saving
1195 while their algorithm returns just 25.75\%. The average of performance
1196 degradation percentage is approximately the same for both algorithms, about 4\%.
1199 For all benchmarks, our algorithm outperforms Spiliopoulos et al. algorithm in
1200 terms of energy and performance trade-off, see Figure~\ref{fig:compare_EDP},
1201 because it maximizes the distance between the energy saving and the performance
1202 degradation values while giving the same weight for both metrics.
1205 \section{Conclusion}
1207 In this paper, a new online frequency selecting algorithm has been presented. It
1208 selects the best possible vector of frequency scaling factors that gives the
1209 maximum distance (optimal trade-off) between the predicted energy and the
1210 predicted performance curves for a heterogeneous platform. This algorithm uses a
1211 new energy model for measuring and predicting the energy of distributed
1212 iterative applications running over heterogeneous platforms. To evaluate the
1213 proposed method, it was applied on the NAS parallel benchmarks and executed over
1214 a heterogeneous platform simulated by SimGrid. The results of the experiments
1215 showed that the algorithm reduces up to 35\% the energy consumption of a message
1216 passing iterative method while limiting the degradation of the performance. The
1217 algorithm also selects different scaling factors according to the percentage of
1218 the computing and communication times, and according to the values of the static
1219 and dynamic powers of the CPUs. Finally, the algorithm was compared to
1220 Spiliopoulos et al. algorithm and the results showed that it outperforms their
1221 algorithm in terms of energy-time trade-off.
1223 In the near future, this method will be applied to real heterogeneous platforms
1224 to evaluate its performance in a real study case. It would also be interesting
1225 to evaluate its scalability over large scale heterogeneous platforms and measure
1226 the energy consumption reduction it can produce. Afterward, we would like to
1227 develop a similar method that is adapted to asynchronous iterative applications
1228 where each task does not wait for other tasks to finish their works. The
1229 development of such a method might require a new energy model because the number
1230 of iterations is not known in advance and depends on the global convergence of
1231 the iterative system.
1233 \section*{Acknowledgment}
1235 This work has been partially supported by the Labex
1236 ACTION project (contract “ANR-11-LABX-01-01”). As a PhD student,
1237 Mr. Ahmed Fanfakh, would like to thank the University of
1238 Babylon (Iraq) for supporting his work.
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1243 % adjust value as needed - may need to be readjusted if
1244 % the document is modified later
1245 %\IEEEtriggeratref{15}
1247 \bibliographystyle{IEEEtran}
1248 \bibliography{IEEEabrv,my_reference}
1251 %%% Local Variables:
1255 %%% ispell-local-dictionary: "american"
1258 % LocalWords: Fanfakh Charr FIXME Tianhe DVFS HPC NAS NPB SMPI Rauber's Rauber
1259 % LocalWords: CMOS EPSA Franche Comté Tflop Rünger IUT Maréchal Juin cedex GPU
1260 % LocalWords: de badri muslim MPI SimGrid GFlops Xeon EP BT GPUs CPUs AMD
1261 % LocalWords: Spiliopoulos scalability