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55 \title{Energy Consumption Reduction for Message Passing Iterative Applications in Heterogeneous Architecture Using DVFS}
65 FEMTO-ST Institute, University of Franche-Comte\\
66 IUT de Belfort-Montbéliard,
67 19 avenue du Maréchal Juin, BP 527, 90016 Belfort cedex, France\\
68 % Telephone: \mbox{+33 3 84 58 77 86}, % Raphaël
69 % Fax: \mbox{+33 3 84 58 77 81}\\ % Dept Info
70 Email: \email{{jean-claude.charr,raphael.couturier,ahmed.fanfakh_badri_muslim,arnaud.giersch}@univ-fcomte.fr}
77 Computing platforms are consuming more and more energy due to the increasing
78 number of nodes composing them. To minimize the operating costs of these
79 platforms many techniques have been used. Dynamic voltage and frequency scaling
80 (DVFS) is one of them. It reduces the frequency of a CPU to lower its energy
81 consumption. However, lowering the frequency of a CPU might increase the
82 execution time of an application running on that processor. Therefore, the
83 frequency that gives the best trade-off between the energy consumption and the
84 performance of an application must be selected.\\
85 In this paper, a new online frequencies selecting algorithm for heterogeneous
86 platforms is presented. It selects the frequency which tries to give the best
87 trade-off between energy saving and performance degradation, for each node
88 computing the message passing iterative application. The algorithm has a small
89 overhead and works without training or profiling. It uses a new energy model for
90 message passing iterative applications running on a heterogeneous platform. The
91 proposed algorithm is evaluated on the SimGrid simulator while running the NAS
92 parallel benchmarks. The experiments show that it reduces the energy
93 consumption by up to 35\% while limiting the performance degradation as much as
94 possible. Finally, the algorithm is compared to an existing method, the
95 comparison results showing that it outperforms the latter.
99 \section{Introduction}
101 The need for more computing power is continually increasing. To partially
102 satisfy this need, most supercomputers constructors just put more computing
103 nodes in their platform. The resulting platforms might achieve higher floating
104 point operations per second (FLOPS), but the energy consumption and the heat
105 dissipation are also increased. As an example, the Chinese supercomputer
106 Tianhe-2 had the highest FLOPS in November 2014 according to the Top500 list
107 \cite{TOP500_Supercomputers_Sites}. However, it was also the most power hungry
108 platform with its over 3 million cores consuming around 17.8 megawatts.
109 Moreover, according to the U.S. annual energy outlook 2014
110 \cite{U.S_Annual.Energy.Outlook.2014}, the price of energy for 1 megawatt-hour
111 was approximately equal to \$70. Therefore, the price of the energy consumed by
112 the Tianhe-2 platform is approximately more than \$10 million each year. The
113 computing platforms must be more energy efficient and offer the highest number
114 of FLOPS per watt possible, such as the L-CSC from the GSI Helmholtz Center
115 which became the top of the Green500 list in November 2014 \cite{Green500_List}.
116 This heterogeneous platform executes more than 5 GFLOPS per watt while consuming
119 Besides platform improvements, there are many software and hardware techniques
120 to lower the energy consumption of these platforms, such as scheduling, DVFS,
121 \dots{} DVFS is a widely used process to reduce the energy consumption of a
122 processor by lowering its frequency
123 \cite{Rizvandi_Some.Observations.on.Optimal.Frequency}. However, it also reduces
124 the number of FLOPS executed by the processor which might increase the execution
125 time of the application running over that processor. Therefore, researchers use
126 different optimization strategies to select the frequency that gives the best
127 trade-off between the energy reduction and performance degradation ratio. In
128 \cite{Our_first_paper}, a frequency selecting algorithm was proposed to reduce
129 the energy consumption of message passing iterative applications running over
130 homogeneous platforms. The results of the experiments show significant energy
131 consumption reductions. In this paper, a new frequency selecting algorithm
132 adapted for heterogeneous platform is presented. It selects the vector of
133 frequencies, for a heterogeneous platform running a message passing iterative
134 application, that simultaneously tries to offer the maximum energy reduction and
135 minimum performance degradation ratio. The algorithm has a very small overhead,
136 works online and does not need any training or profiling.
138 This paper is organized as follows: Section~\ref{sec.relwork} presents some
139 related works from other authors. Section~\ref{sec.exe} describes how the
140 execution time of message passing programs can be predicted. It also presents an energy
141 model that predicts the energy consumption of an application running over a heterogeneous platform. Section~\ref{sec.compet} presents
142 the energy-performance objective function that maximizes the reduction of energy
143 consumption while minimizing the degradation of the program's performance.
144 Section~\ref{sec.optim} details the proposed frequency selecting algorithm then the precision of the proposed algorithm is verified.
145 Section~\ref{sec.expe} presents the results of applying the algorithm on the NAS parallel benchmarks and executing them
146 on a heterogeneous platform. It shows the results of running three
147 different power scenarios and comparing them. Moreover, it also shows the comparison results
148 between the proposed method and an existing method.
149 Finally, in Section~\ref{sec.concl} the paper ends with a summary and some future works.
151 \section{Related works}
153 DVFS is a technique used in modern processors to scale down both the voltage and
154 the frequency of the CPU while computing, in order to reduce the energy
155 consumption of the processor. DVFS is also allowed in GPUs to achieve the same
156 goal. Reducing the frequency of a processor lowers its number of FLOPS and might
157 degrade the performance of the application running on that processor, especially
158 if it is compute bound. Therefore selecting the appropriate frequency for a
159 processor to satisfy some objectives while taking into account all the
160 constraints, is not a trivial operation. Many researchers used different
161 strategies to tackle this problem. Some of them developed online methods that
162 compute the new frequency while executing the application, such
163 as~\cite{Hao_Learning.based.DVFS,Spiliopoulos_Green.governors.Adaptive.DVFS}.
164 Others used offline methods that might need to run the application and profile
165 it before selecting the new frequency, such
166 as~\cite{Rountree_Bounding.energy.consumption.in.MPI,Cochran_Pack_and_Cap_Adaptive_DVFS}.
167 The methods could be heuristics, exact or brute force methods that satisfy
168 varied objectives such as energy reduction or performance. They also could be
169 adapted to the execution's environment and the type of the application such as
170 sequential, parallel or distributed architecture, homogeneous or heterogeneous
171 platform, synchronous or asynchronous application, \dots{}
173 In this paper, we are interested in reducing energy for message passing iterative synchronous applications running over heterogeneous platforms.
174 Some works have already been done for such platforms and they can be classified into two types of heterogeneous platforms:
177 \item the platform is composed of homogeneous GPUs and homogeneous CPUs.
178 \item the platform is only composed of heterogeneous CPUs.
182 For the first type of platform, the computing intensive parallel tasks are
183 executed on the GPUs and the rest are executed on the CPUs. Luley et
184 al.~\cite{Luley_Energy.efficiency.evaluation.and.benchmarking}, proposed a
185 heterogeneous cluster composed of Intel Xeon CPUs and NVIDIA GPUs. Their main
186 goal was to maximize the energy efficiency of the platform during computation by
187 maximizing the number of FLOPS per watt generated.
188 In~\cite{KaiMa_Holistic.Approach.to.Energy.Efficiency.in.GPU-CPU}, Kai Ma et
189 al. developed a scheduling algorithm that distributes workloads proportional to
190 the computing power of the nodes which could be a GPU or a CPU. All the tasks
191 must be completed at the same time. In~\cite{Rong_Effects.of.DVFS.on.K20.GPU},
192 Rong et al. showed that a heterogeneous (GPUs and CPUs) cluster that enables
193 DVFS gave better energy and performance efficiency than other clusters only
196 The work presented in this paper concerns the second type of platform, with
197 heterogeneous CPUs. Many methods were conceived to reduce the energy
198 consumption of this type of platform. Naveen et
199 al.~\cite{Naveen_Power.Efficient.Resource.Scaling} developed a method that
200 minimizes the value of $energy\cdot delay^2$ (the delay is the sum of slack
201 times that happen during synchronous communications) by dynamically assigning
202 new frequencies to the CPUs of the heterogeneous cluster. Lizhe et
203 al.~\cite{Lizhe_Energy.aware.parallel.task.scheduling} proposed an algorithm
204 that divides the executed tasks into two types: the critical and non critical
205 tasks. The algorithm scales down the frequency of non critical tasks
206 proportionally to their slack and communication times while limiting the
207 performance degradation percentage to less than
208 10\%. In~\cite{Joshi_Blackbox.prediction.of.impact.of.DVFS}, they developed a
209 heterogeneous cluster composed of two types of Intel and AMD processors. They
210 use a gradient method to predict the impact of DVFS operations on performance.
211 In~\cite{Shelepov_Scheduling.on.Heterogeneous.Multicore} and
212 \cite{Li_Minimizing.Energy.Consumption.for.Frame.Based.Tasks}, the best
213 frequencies for a specified heterogeneous cluster are selected offline using
214 some heuristic. Chen et
215 al.~\cite{Chen_DVFS.under.quality.of.service.requirements} used a greedy dynamic
216 programming approach to minimize the power consumption of heterogeneous servers
217 while respecting given time constraints. This approach had considerable
218 overhead. In contrast to the above described papers, this paper presents the
219 following contributions :
221 \item two new energy and performance models for message passing iterative synchronous applications running over
222 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.
224 \item a new online frequency selecting algorithm for heterogeneous platforms. The algorithm has a very small
225 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.
229 \section{The performance and energy consumption measurements on heterogeneous architecture}
234 \subsection{The execution time of message passing distributed
235 iterative applications on a heterogeneous platform}
237 In this paper, we are interested in reducing the energy consumption of message
238 passing distributed iterative synchronous applications running over
239 heterogeneous platforms. A heterogeneous platform is defined as a collection of
240 heterogeneous computing nodes interconnected via a high speed homogeneous
241 network. Therefore, each node has different characteristics such as computing
242 power (FLOPS), energy consumption, CPU's frequency range, \dots{} but they all
243 have the same network bandwidth and latency.
245 The overall execution time of a distributed iterative synchronous application
246 over a heterogeneous platform consists of the sum of the computation time and
247 the communication time for every iteration on a node. However, due to the
248 heterogeneous computation power of the computing nodes, slack times might occur
249 when fast nodes have to wait, during synchronous communications, for the slower
250 nodes to finish their computations (see Figure~\ref{fig:heter}). Therefore, the
251 overall execution time of the program is the execution time of the slowest task
252 which has the highest computation time and no slack time.
256 \includegraphics[scale=0.6]{fig/commtasks}
257 \caption{Parallel tasks on a heterogeneous platform}
261 Dynamic Voltage and Frequency Scaling (DVFS) is a process, implemented in
262 modern processors, that reduces the energy consumption of a CPU by scaling
263 down its voltage and frequency. Since DVFS lowers the frequency of a CPU
264 and consequently its computing power, the execution time of a program running
265 over that scaled down processor might increase, especially if the program is
266 compute bound. The frequency reduction process can be expressed by the scaling
267 factor S which is the ratio between the maximum and the new frequency of a CPU
271 S = \frac{F_\textit{max}}{F_\textit{new}}
273 The execution time of a compute bound sequential program is linearly proportional
274 to the frequency scaling factor $S$. On the other hand, message passing
275 distributed applications consist of two parts: computation and communication.
276 The execution time of the computation part is linearly proportional to the
277 frequency scaling factor $S$ but the communication time is not affected by the
278 scaling factor because the processors involved remain idle during the
279 communications~\cite{Freeh_Exploring.the.Energy.Time.Tradeoff}.
280 The communication time for a task is the summation of periods of
281 time that begin with an MPI call for sending or receiving a message
282 until the message is synchronously sent or received.
284 Since in a heterogeneous platform each node has different characteristics,
285 especially different frequency gears, when applying DVFS operations on these
286 nodes, they may get different scaling factors represented by a scaling vector:
287 $(S_1, S_2,\dots, S_N)$ where $S_i$ is the scaling factor of processor $i$. To
288 be able to predict the execution time of message passing synchronous iterative
289 applications running over a heterogeneous platform, for different vectors of
290 scaling factors, the communication time and the computation time for all the
291 tasks must be measured during the first iteration before applying any DVFS
292 operation. Then the execution time for one iteration of the application with any
293 vector of scaling factors can be predicted using (\ref{eq:perf}).
296 \textit T_\textit{new} =
297 \max_{i=1,2,\dots,N} ({TcpOld_{i}} \cdot S_{i}) + MinTcm
302 MinTcm = \min_{i=1,2,\dots,N} (Tcm_i)
304 where $TcpOld_i$ is the computation time of processor $i$ during the first
305 iteration and $MinTcm$ is the communication time of the slowest processor from
306 the first iteration. The model computes the maximum computation time with
307 scaling factor from each node added to the communication time of the slowest
308 node. It means only the communication time without any slack time is taken into
309 account. Therefore, the execution time of the iterative application is equal to
310 the execution time of one iteration as in (\ref{eq:perf}) multiplied by the
311 number of iterations of that application.
313 This prediction model is developed from the model to predict the execution time
314 of message passing distributed applications for homogeneous
315 architectures~\cite{Our_first_paper}. The execution time prediction model is
316 used in the method to optimize both the energy consumption and the performance of
317 iterative methods, which is presented in the following sections.
320 \subsection{Energy model for heterogeneous platform}
321 Many researchers~\cite{Malkowski_energy.efficient.high.performance.computing,
322 Rauber_Analytical.Modeling.for.Energy,Zhuo_Energy.efficient.Dynamic.Task.Scheduling,
323 Rizvandi_Some.Observations.on.Optimal.Frequency} divide the power consumed by a processor into
324 two power metrics: the static and the dynamic power. While the first one is
325 consumed as long as the computing unit is turned on, the latter is only consumed during
326 computation times. The dynamic power $Pd$ is related to the switching
327 activity $\alpha$, load capacitance $C_L$, the supply voltage $V$ and
328 operational frequency $F$, as shown in (\ref{eq:pd}).
331 Pd = \alpha \cdot C_L \cdot V^2 \cdot F
333 The static power $Ps$ captures the leakage power as follows:
336 Ps = V \cdot N_{trans} \cdot K_{design} \cdot I_{leak}
338 where V is the supply voltage, $N_{trans}$ is the number of transistors,
339 $K_{design}$ is a design dependent parameter and $I_{leak}$ is a
340 technology dependent parameter. The energy consumed by an individual processor
341 to execute a given program can be computed as:
344 E_\textit{ind} = Pd \cdot Tcp + Ps \cdot T
346 where $T$ is the execution time of the program, $Tcp$ is the computation
347 time and $Tcp \le T$. $Tcp$ may be equal to $T$ if there is no
348 communication and no slack time.
350 The main objective of DVFS operation is to reduce the overall energy consumption~\cite{Le_DVFS.Laws.of.Diminishing.Returns}.
351 The operational frequency $F$ depends linearly on the supply voltage $V$, i.e., $V = \beta \cdot F$ with some
352 constant $\beta$.~This equation is used to study the change of the dynamic
353 voltage with respect to various frequency values in~\cite{Rauber_Analytical.Modeling.for.Energy}. The reduction
354 process of the frequency can be expressed by the scaling factor $S$ which is the
355 ratio between the maximum and the new frequency as in (\ref{eq:s}).
356 The CPU governors are power schemes supplied by the operating
357 system's kernel to lower a core's frequency. The new frequency
358 $F_{new}$ from (\ref{eq:s}) can be calculated as follows:
361 F_\textit{new} = S^{-1} \cdot F_\textit{max}
363 Replacing $F_{new}$ in (\ref{eq:pd}) as in (\ref{eq:fnew}) gives the following
364 equation for dynamic power consumption:
367 {P}_\textit{dNew} = \alpha \cdot C_L \cdot V^2 \cdot F_{new} = \alpha \cdot C_L \cdot \beta^2 \cdot F_{new}^3 \\
368 {} = \alpha \cdot C_L \cdot V^2 \cdot F_{max} \cdot S^{-3} = P_{dOld} \cdot S^{-3}
370 where $ {P}_\textit{dNew}$ and $P_{dOld}$ are the dynamic power consumed with the
371 new frequency and the maximum frequency respectively.
373 According to (\ref{eq:pdnew}) the dynamic power is reduced by a factor of $S^{-3}$ when
374 reducing the frequency by a factor of $S$~\cite{Rauber_Analytical.Modeling.for.Energy}. Since the FLOPS of a CPU is proportional
375 to the frequency of a CPU, the computation time is increased proportionally to $S$.
376 The new dynamic energy is the dynamic power multiplied by the new time of computation
377 and is given by the following equation:
380 E_\textit{dNew} = P_{dOld} \cdot S^{-3} \cdot (Tcp \cdot S)= S^{-2}\cdot P_{dOld} \cdot Tcp
382 The static power is related to the power leakage of the CPU and is consumed during computation
383 and even when idle. As in~\cite{Rauber_Analytical.Modeling.for.Energy,Zhuo_Energy.efficient.Dynamic.Task.Scheduling},
384 the static power of a processor is considered as constant
385 during idle and computation periods, and for all its available frequencies.
386 The static energy is the static power multiplied by the execution time of the program.
387 According to the execution time model in (\ref{eq:perf}), the execution time of the program
388 is the sum of the computation and the communication times. The computation time is linearly related
389 to the frequency scaling factor, while this scaling factor does not affect the communication time.
390 The static energy of a processor after scaling its frequency is computed as follows:
393 E_\textit{s} = Ps \cdot (Tcp \cdot S + Tcm)
396 In the considered heterogeneous platform, each processor $i$ might have
397 different dynamic and static powers, noted as $Pd_{i}$ and $Ps_{i}$
398 respectively. Therefore, even if the distributed message passing iterative
399 application is load balanced, the computation time of each CPU $i$ noted
400 $Tcp_{i}$ might be different and different frequency scaling factors might be
401 computed in order to decrease the overall energy consumption of the application
402 and reduce slack times. The communication time of a processor $i$ is noted as
403 $Tcm_{i}$ and could contain slack times when communicating with slower
404 nodes, see Figure~\ref{fig:heter}. Therefore, all nodes do not have equal
405 communication times. While the dynamic energy is computed according to the
406 frequency scaling factor and the dynamic power of each node as in
407 (\ref{eq:Edyn}), the static energy is computed as the sum of the execution time
408 of one iteration multiplied by the static power of each processor. The overall
409 energy consumption of a message passing distributed application executed over a
410 heterogeneous platform during one iteration is the summation of all dynamic and
411 static energies for each processor. It is computed as follows:
414 E = \sum_{i=1}^{N} {(S_i^{-2} \cdot Pd_{i} \cdot Tcp_i)} + {} \\
415 \sum_{i=1}^{N} (Ps_{i} \cdot (\max_{i=1,2,\dots,N} (Tcp_i \cdot S_{i}) +
419 Reducing the frequencies of the processors according to the vector of
420 scaling factors $(S_1, S_2,\dots, S_N)$ may degrade the performance of the
421 application and thus, increase the static energy because the execution time is
422 increased~\cite{Kim_Leakage.Current.Moore.Law}. The overall energy consumption for the iterative
423 application can be measured by measuring the energy consumption for one iteration as in (\ref{eq:energy})
424 multiplied by the number of iterations of that application.
427 \section{Optimization of both energy consumption and performance}
430 Using the lowest frequency for each processor does not necessarily give the most
431 energy efficient execution of an application. Indeed, even though the dynamic
432 power is reduced while scaling down the frequency of a processor, its
433 computation power is proportionally decreased. Hence, the execution time might
434 be drastically increased and during that time, dynamic and static powers are
435 being consumed. Therefore, it might cancel any gains achieved by scaling down
436 the frequency of all nodes to the minimum and the overall energy consumption of
437 the application might not be the optimal one. It is not trivial to select the
438 appropriate frequency scaling factor for each processor while considering the
439 characteristics of each processor (computation power, range of frequencies,
440 dynamic and static powers) and the task executed (computation/communication
441 ratio). The aim being to reduce the overall energy consumption and to avoid
442 increasing significantly the execution time. In our previous
443 work~\cite{Our_first_paper}, we proposed a method that selects the optimal
444 frequency scaling factor for a homogeneous cluster executing a message passing
445 iterative synchronous application while giving the best trade-off between the
446 energy consumption and the performance for such applications. In this work we
447 are interested in heterogeneous clusters as described above. Due to the
448 heterogeneity of the processors, a vector of scaling factors should
449 be selected and it must give the best trade-off between energy consumption and
452 The relation between the energy consumption and the execution time for an
453 application is complex and nonlinear, Thus, unlike the relation between the
454 execution time and the scaling factor, the relation between the energy and the
455 frequency scaling factors is nonlinear, for more details refer
456 to~\cite{Freeh_Exploring.the.Energy.Time.Tradeoff}. Moreover, these relations
457 are not measured using the same metric. To solve this problem, the execution
458 time is normalized by computing the ratio between the new execution time (after
459 scaling down the frequencies of some processors) and the initial one (with
460 maximum frequency for all nodes) as follows:
463 P_\textit{Norm} = \frac{T_\textit{New}}{T_\textit{Old}}\\
464 {} = \frac{ \max_{i=1,2,\dots,N} (Tcp_{i} \cdot S_{i}) +MinTcm}
465 {\max_{i=1,2,\dots,N}{(Tcp_i+Tcm_i)}}
469 In the same way, the energy is normalized by computing the ratio between the consumed energy
470 while scaling down the frequency and the consumed energy with maximum frequency for all nodes:
473 E_\textit{Norm} = \frac{E_\textit{Reduced}}{E_\textit{Original}} \\
474 {} = \frac{ \sum_{i=1}^{N}{(S_i^{-2} \cdot Pd_i \cdot Tcp_i)} +
475 \sum_{i=1}^{N} {(Ps_i \cdot T_{New})}}{\sum_{i=1}^{N}{( Pd_i \cdot Tcp_i)} +
476 \sum_{i=1}^{N} {(Ps_i \cdot T_{Old})}}
478 Where $E_\textit{Reduced}$ and $E_\textit{Original}$ are computed using (\ref{eq:energy}) and
479 $T_{New}$ and $T_{Old}$ are computed as in (\ref{eq:pnorm}).
482 goal is to optimize the energy and execution time at the same time, the normalized
483 energy and execution time curves are not in the same direction. According
484 to the equations~(\ref{eq:pnorm}) and (\ref{eq:enorm}), the vector of frequency
485 scaling factors $S_1,S_2,\dots,S_N$ reduce both the energy and the execution
486 time simultaneously. But the main objective is to produce maximum energy
487 reduction with minimum execution time reduction.
489 This problem can be solved by making the optimization process for energy and
490 execution time following the same direction. Therefore, the equation of the
491 normalized execution time is inverted which gives the normalized performance equation, as follows:
494 P_\textit{Norm} = \frac{T_\textit{Old}}{T_\textit{New}}\\
495 = \frac{\max_{i=1,2,\dots,N}{(Tcp_i+Tcm_i)}}
496 { \max_{i=1,2,\dots,N} (Tcp_{i} \cdot S_{i}) + MinTcm}
502 \subfloat[Homogeneous platform]{%
503 \includegraphics[width=.33\textwidth]{fig/homo}\label{fig:r1}}%
506 \subfloat[Heterogeneous platform]{%
507 \includegraphics[width=.33\textwidth]{fig/heter}\label{fig:r2}}
509 \caption{The energy and performance relation}
512 Then, the objective function can be modeled in order to find the maximum
513 distance between the energy curve (\ref{eq:enorm}) and the performance curve
514 (\ref{eq:pnorm_inv}) over all available sets of scaling factors. This
515 represents the minimum energy consumption with minimum execution time (maximum
516 performance) at the same time, see Figure~\ref{fig:r1} or
517 Figure~\ref{fig:r2}. Then the objective function has the following form:
521 \max_{i=1,\dots F, j=1,\dots,N}
522 (\overbrace{P_\textit{Norm}(S_{ij})}^{\text{Maximize}} -
523 \overbrace{E_\textit{Norm}(S_{ij})}^{\text{Minimize}} )
525 where $N$ is the number of nodes and $F$ is the number of available frequencies for each node.
526 Then, the optimal set of scaling factors that satisfies (\ref{eq:max}) can be selected.
527 The objective function can work with any energy model or any power values for each node
528 (static and dynamic powers). However, the most important energy reduction gain can be achieved when
529 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}.
531 \section{The scaling factors selection algorithm for heterogeneous platforms }
534 \subsection{The algorithm details}
535 In this section, Algorithm~\ref{HSA} is presented. It selects the frequency
536 scaling factors vector that gives the best trade-off between minimizing the
537 energy consumption and maximizing the performance of a message passing
538 synchronous iterative application executed on a heterogeneous platform. It works
539 online during the execution time of the iterative message passing program. It
540 uses information gathered during the first iteration such as the computation
541 time and the communication time in one iteration for each node. The algorithm is
542 executed after the first iteration and returns a vector of optimal frequency
543 scaling factors that satisfies the objective function (\ref{eq:max}). The
544 program applies DVFS operations to change the frequencies of the CPUs according
545 to the computed scaling factors. This algorithm is called just once during the
546 execution of the program. Algorithm~\ref{dvfs} shows where and when the proposed
547 scaling algorithm is called in the iterative MPI program.
549 The nodes in a heterogeneous platform have different computing powers, thus
550 while executing message passing iterative synchronous applications, fast nodes
551 have to wait for the slower ones to finish their computations before being able
552 to synchronously communicate with them as in Figure~\ref{fig:heter}. These
553 periods are called idle or slack times. The algorithm takes into account this
554 problem and tries to reduce these slack times when selecting the frequency
555 scaling factors vector. At first, it selects initial frequency scaling factors
556 that increase the execution times of fast nodes and minimize the differences
557 between the computation times of fast and slow nodes. The value of the initial
558 frequency scaling factor for each node is inversely proportional to its
559 computation time that was gathered from the first iteration. These initial
560 frequency scaling factors are computed as a ratio between the computation time
561 of the slowest node and the computation time of the node $i$ as follows:
564 Scp_{i} = \frac{\max_{i=1,2,\dots,N}(Tcp_i)}{Tcp_i}
566 Using the initial frequency scaling factors computed in (\ref{eq:Scp}), the algorithm computes
567 the initial frequencies for all nodes as a ratio between the maximum frequency of node $i$
568 and the computation scaling factor $Scp_i$ as follows:
571 F_{i} = \frac{Fmax_i}{Scp_i},~{i=1,2,\cdots,N}
573 If the computed initial frequency for a node is not available in the gears of
574 that node, it is replaced by the nearest available frequency. In
575 Figure~\ref{fig:st_freq}, the nodes are sorted by their computing power in
576 ascending order and the frequencies of the faster nodes are scaled down
577 according to the computed initial frequency scaling factors. The resulting new
578 frequencies are colored in blue in Figure~\ref{fig:st_freq}. This set of
579 frequencies can be considered as a higher bound for the search space of the
580 optimal vector of frequencies because selecting frequency scaling factors higher
581 than the higher bound will not improve the performance of the application and it
582 will increase its overall energy consumption. Therefore the algorithm that
583 selects the frequency scaling factors starts the search method from these
584 initial frequencies and takes a downward search direction toward lower
585 frequencies. The algorithm iterates on all left frequencies, from the higher
586 bound until all nodes reach their minimum frequencies, to compute their overall
587 energy consumption and performance, and select the optimal frequency scaling
588 factors vector. At each iteration the algorithm determines the slowest node
589 according to the equation (\ref{eq:perf}) and keeps its frequency unchanged,
590 while it lowers the frequency of all other nodes by one gear. The new overall
591 energy consumption and execution time are computed according to the new scaling
592 factors. The optimal set of frequency scaling factors is the set that gives the
593 highest distance according to the objective function (\ref{eq:max}).
595 Figures~\ref{fig:r1} and \ref{fig:r2} illustrate the normalized performance and
596 consumed energy for an application running on a homogeneous platform and a
597 heterogeneous platform respectively while increasing the scaling factors. It can
598 be noticed that in a homogeneous platform the search for the optimal scaling
599 factor should start from the maximum frequency because the performance and the
600 consumed energy decrease from the beginning of the plot. On the other hand,
601 in the heterogeneous platform the performance is maintained at the beginning of
602 the plot even if the frequencies of the faster nodes decrease until the
603 computing power of scaled down nodes are lower than the slowest node. In other
604 words, until they reach the higher bound. It can also be noticed that the higher
605 the difference between the faster nodes and the slower nodes is, the bigger the
606 maximum distance between the energy curve and the performance curve is while
607 the scaling factors are varying which results in bigger energy savings.
610 \includegraphics[scale=0.5]{fig/start_freq}
611 \caption{Selecting the initial frequencies}
619 \begin{algorithmic}[1]
623 \item[$Tcp_i$] array of all computation times for all nodes during one iteration and with highest frequency.
624 \item[$Tcm_i$] array of all communication times for all nodes during one iteration and with highest frequency.
625 \item[$Fmax_i$] array of the maximum frequencies for all nodes.
626 \item[$Pd_i$] array of the dynamic powers for all nodes.
627 \item[$Ps_i$] array of the static powers for all nodes.
628 \item[$Fdiff_i$] array of the difference between two successive frequencies for all nodes.
630 \Ensure $Sopt_1,Sopt_2 \dots, Sopt_N$ is a vector of optimal scaling factors
632 \State $ Scp_i \gets \frac{\max_{i=1,2,\dots,N}(Tcp_i)}{Tcp_i} $
633 \State $F_{i} \gets \frac{Fmax_i}{Scp_i},~{i=1,2,\cdots,N}$
634 \State Round the computed initial frequencies $F_i$ to the closest one available in each node.
635 \If{(not the first frequency)}
636 \State $F_i \gets F_i+Fdiff_i,~i=1,\dots,N.$
638 \State $T_\textit{Old} \gets max_{~i=1,\dots,N } (Tcp_i+Tcm_i)$
639 \State $E_\textit{Original} \gets \sum_{i=1}^{N}{( Pd_i \cdot Tcp_i)} +\sum_{i=1}^{N} {(Ps_i \cdot T_{Old})}$
640 \State $Sopt_{i} \gets 1,~i=1,\dots,N. $
641 \State $Dist \gets 0 $
642 \While {(all nodes not reach their minimum frequency)}
643 \If{(not the last freq. \textbf{and} not the slowest node)}
644 \State $F_i \gets F_i - Fdiff_i,~i=1,\dots,N.$
645 \State $S_i \gets \frac{Fmax_i}{F_i},~i=1,\dots,N.$
647 \State $T_{New} \gets max_\textit{~i=1,\dots,N} (Tcp_{i} \cdot S_{i}) + MinTcm $
648 \State $E_\textit{Reduced} \gets \sum_{i=1}^{N}{(S_i^{-2} \cdot Pd_i \cdot Tcp_i)} + $ \hspace*{43 mm}
649 $\sum_{i=1}^{N} {(Ps_i \cdot T_{New})} $
650 \State $ P_\textit{Norm} \gets \frac{T_\textit{Old}}{T_\textit{New}}$
651 \State $E_\textit{Norm}\gets \frac{E_\textit{Reduced}}{E_\textit{Original}}$
652 \If{$(\Pnorm - \Enorm > \Dist)$}
653 \State $Sopt_{i} \gets S_{i},~i=1,\dots,N. $
654 \State $\Dist \gets \Pnorm - \Enorm$
657 \State Return $Sopt_1,Sopt_2,\dots,Sopt_N$
659 \caption{frequency scaling factors selection algorithm}
664 \begin{algorithmic}[1]
666 \For {$k=1$ to \textit{some iterations}}
667 \State Computations section.
668 \State Communications section.
670 \State Gather all times of computation and\newline\hspace*{3em}%
671 communication from each node.
672 \State Call Algorithm \ref{HSA}.
673 \State Compute the new frequencies from the\newline\hspace*{3em}%
674 returned optimal scaling factors.
675 \State Set the new frequencies to nodes.
679 \caption{DVFS algorithm}
683 \subsection{The evaluation of the proposed algorithm}
684 \label{sec.verif.algo}
685 The precision of the proposed algorithm mainly depends on the execution time
686 prediction model defined in (\ref{eq:perf}) and the energy model computed by
687 (\ref{eq:energy}). The energy model is also significantly dependent on the
688 execution time model because the static energy is linearly related to the
689 execution time and the dynamic energy is related to the computation time. So,
690 all the works presented in this paper are based on the execution time model. To
691 verify this model, the predicted execution time was compared to the real
692 execution time over SimGrid/SMPI simulator,
693 v3.10~\cite{casanova+giersch+legrand+al.2014.versatile}, for all the NAS
694 parallel benchmarks NPB v3.3 \cite{NAS.Parallel.Benchmarks}, running class B on
695 8 or 9 nodes. The comparison showed that the proposed execution time model is
696 very precise, the maximum normalized difference between the predicted execution
697 time and the real execution time is equal to 0.03 for all the NAS benchmarks.
699 Since the proposed algorithm is not an exact method it does not test all the
700 possible solutions (vectors of scaling factors) in the search space. To prove
701 its efficiency, it was compared on small instances to a brute force search
702 algorithm that tests all the possible solutions. The brute force algorithm was
703 applied to different NAS benchmarks classes with different number of nodes. The
704 solutions returned by the brute force algorithm and the proposed algorithm were
705 identical and the proposed algorithm was on average 10 times faster than the
706 brute force algorithm. It has a small execution time: for a heterogeneous
707 cluster composed of four different types of nodes having the characteristics
708 presented in Table~\ref{table:platform}, it takes on average \np[ms]{0.04} for 4
709 nodes and \np[ms]{0.15} on average for 144 nodes to compute the best scaling
710 factors vector. The algorithm complexity is $O(F\cdot (N \cdot4) )$, where $F$
711 is the number of iterations and $N$ is the number of computing nodes. The
712 algorithm needs from 12 to 20 iterations to select the best vector of frequency
713 scaling factors that gives the results of the next sections.
715 \section{Experimental results}
717 To evaluate the efficiency and the overall energy consumption reduction of
718 Algorithm~\ref{HSA}, it was applied to the NAS parallel benchmarks NPB v3.3. The
719 experiments were executed on the simulator SimGrid/SMPI which offers easy tools
720 to create a heterogeneous platform and run message passing applications over it.
721 The heterogeneous platform that was used in the experiments, had one core per
722 node because just one process was executed per node. The heterogeneous platform
723 was composed of four types of nodes. Each type of nodes had different
724 characteristics such as the maximum CPU frequency, the number of available
725 frequencies and the computational power, see Table~\ref{table:platform}. The
726 characteristics of these different types of nodes are inspired from the
727 specifications of real Intel processors. The heterogeneous platform had up to
728 144 nodes and had nodes from the four types in equal proportions, for example if
729 a benchmark was executed on 8 nodes, 2 nodes from each type were used. Since the
730 constructors of CPUs do not specify the dynamic and the static power of their
731 CPUs, for each type of node they were chosen proportionally to its computing
732 power (FLOPS). In the initial heterogeneous platform, while computing with
733 highest frequency, each node consumed an amount of power proportional to its
734 computing power (which corresponds to 80\% of its dynamic power and the
735 remaining 20\% to the static power), the same assumption was made in
736 \cite{Our_first_paper,Rauber_Analytical.Modeling.for.Energy}. Finally, These
737 nodes were connected via an Ethernet network with 1 Gbit/s bandwidth.
741 \caption{Heterogeneous nodes characteristics}
744 \begin{tabular}{|*{7}{l|}}
746 Node &Simulated & Max & Min & Diff. & Dynamic & Static \\
747 type &GFLOPS & Freq. & Freq. & Freq. & power & power \\
748 & & GHz & GHz &GHz & & \\
750 1 &40 & 2.5 & 1.2 & 0.1 & 20~W &4~W \\
753 2 &50 & 2.66 & 1.6 & 0.133 & 25~W &5~W \\
756 3 &60 & 2.9 & 1.2 & 0.1 & 30~W &6~W \\
759 4 &70 & 3.4 & 1.6 & 0.133 & 35~W &7~W \\
763 \label{table:platform}
767 %\subsection{Performance prediction verification}
770 \subsection{The experimental results of the scaling algorithm}
774 The proposed algorithm was applied to the seven parallel NAS benchmarks (EP, CG,
775 MG, FT, BT, LU and SP) and the benchmarks were executed with the three classes:
776 A, B and C. However, due to the lack of space in this paper, only the results of
777 the biggest class, C, are presented while being run on different number of
778 nodes, ranging from 4 to 128 or 144 nodes depending on the benchmark being
779 executed. Indeed, the benchmarks CG, MG, LU, EP and FT had to be executed on $1,
780 2, 4, 8, 16, 32, 64, 128$ nodes. The other benchmarks such as BT and SP had to
781 be executed on $1, 4, 9, 16, 36, 64, 144$ nodes.
786 \caption{Running NAS benchmarks on 4 nodes }
789 \begin{tabular}{|*{7}{r|}}
792 Program & Execution & Energy & Energy & Performance & Distance \\
793 name & time/s & consumption/J & saving\% & degradation\% & \\
795 CG & 64.64 & 3560.39 &34.16 &6.72 &27.44 \\
797 MG & 18.89 & 1074.87 &35.37 &4.34 &31.03 \\
799 EP &79.73 &5521.04 &26.83 &3.04 &23.79 \\
801 LU &308.65 &21126.00 &34.00 &6.16 &27.84 \\
803 BT &360.12 &21505.55 &35.36 &8.49 &26.87 \\
805 SP &234.24 &13572.16 &35.22 &5.70 &29.52 \\
807 FT &81.58 &4151.48 &35.58 &0.99 &34.59 \\
815 \caption{Running NAS benchmarks on 8 and 9 nodes }
818 \begin{tabular}{|*{7}{r|}}
821 Program & Execution & Energy & Energy & Performance & Distance \\
822 name & time/s & consumption/J & saving\% & degradation\% & \\
824 CG &36.11 &3263.49 &31.25 &7.12 &24.13 \\
826 MG &8.99 &953.39 &33.78 &6.41 &27.37 \\
828 EP &40.39 &5652.81 &27.04 &0.49 &26.55 \\
830 LU &218.79 &36149.77 &28.23 &0.01 &28.22 \\
832 BT &166.89 &23207.42 &32.32 &7.89 &24.43 \\
834 SP &104.73 &18414.62 &24.73 &2.78 &21.95 \\
836 FT &51.10 &4913.26 &31.02 &2.54 &28.48 \\
844 \caption{Running NAS benchmarks on 16 nodes }
847 \begin{tabular}{|*{7}{r|}}
850 Program & Execution & Energy & Energy & Performance & Distance \\
851 name & time/s & consumption/J & saving\% & degradation\% & \\
853 CG &31.74 &4373.90 &26.29 &9.57 &16.72 \\
855 MG &5.71 &1076.19 &32.49 &6.05 &26.44 \\
857 EP &20.11 &5638.49 &26.85 &0.56 &26.29 \\
859 LU &144.13 &42529.06 &28.80 &6.56 &22.24 \\
861 BT &97.29 &22813.86 &34.95 &5.80 &29.15 \\
863 SP &66.49 &20821.67 &22.49 &3.82 &18.67 \\
865 FT &37.01 &5505.60 &31.59 &6.48 &25.11 \\
868 \label{table:res_16n}
873 \caption{Running NAS benchmarks on 32 and 36 nodes }
876 \begin{tabular}{|*{7}{r|}}
879 Program & Execution & Energy & Energy & Performance & Distance \\
880 name & time/s & consumption/J & saving\% & degradation\% & \\
882 CG &32.35 &6704.21 &16.15 &5.30 &10.85 \\
884 MG &4.30 &1355.58 &28.93 &8.85 &20.08 \\
886 EP &9.96 &5519.68 &26.98 &0.02 &26.96 \\
888 LU &99.93 &67463.43 &23.60 &2.45 &21.15 \\
890 BT &48.61 &23796.97 &34.62 &5.83 &28.79 \\
892 SP &46.01 &27007.43 &22.72 &3.45 &19.27 \\
894 FT &28.06 &7142.69 &23.09 &2.90 &20.19 \\
897 \label{table:res_32n}
902 \caption{Running NAS benchmarks on 64 nodes }
905 \begin{tabular}{|*{7}{r|}}
908 Program & Execution & Energy & Energy & Performance & Distance \\
909 name & time/s & consumption/J & saving\% & degradation\% & \\
911 CG &46.65 &17521.83 &8.13 &1.68 &6.45 \\
913 MG &3.27 &1534.70 &29.27 &14.35 &14.92 \\
915 EP &5.05 &5471.1084 &27.12 &3.11 &24.01 \\
917 LU &73.92 &101339.16 &21.96 &3.67 &18.29 \\
919 BT &39.99 &27166.71 &32.02 &12.28 &19.74 \\
921 SP &52.00 &49099.28 &24.84 &0.03 &24.81 \\
923 FT &25.97 &10416.82 &20.15 &4.87 &15.28 \\
926 \label{table:res_64n}
931 \caption{Running NAS benchmarks on 128 and 144 nodes }
934 \begin{tabular}{|*{7}{r|}}
937 Program & Execution & Energy & Energy & Performance & Distance \\
938 name & time/s & consumption/J & saving\% & degradation\% & \\
940 CG &56.92 &41163.36 &4.00 &1.10 &2.90 \\
942 MG &3.55 &2843.33 &18.77 &10.38 &8.39 \\
944 EP &2.67 &5669.66 &27.09 &0.03 &27.06 \\
946 LU &51.23 &144471.90 &16.67 &2.36 &14.31 \\
948 BT &37.96 &44243.82 &23.18 &1.28 &21.90 \\
950 SP &64.53 &115409.71 &26.72 &0.05 &26.67 \\
952 FT &25.51 &18808.72 &12.85 &2.84 &10.01 \\
955 \label{table:res_128n}
957 The overall energy consumption was computed for each instance according to the
958 energy consumption model (\ref{eq:energy}), with and without applying the
959 algorithm. The execution time was also measured for all these experiments. Then,
960 the energy saving and performance degradation percentages were computed for each
961 instance. The results are presented in Tables~\ref{table:res_4n},
962 \ref{table:res_8n}, \ref{table:res_16n}, \ref{table:res_32n},
963 \ref{table:res_64n} and \ref{table:res_128n}. All these results are the average
964 values from many experiments for energy savings and performance degradation.
965 The tables show the experimental results for running the NAS parallel benchmarks
966 on different number of nodes. The experiments show that the algorithm
967 significantly reduces the energy consumption (up to 35\%) and tries to limit the
968 performance degradation. They also show that the energy saving percentage
969 decreases when the number of computing nodes increases. This reduction is due
970 to the increase of the communication times compared to the execution times when
971 the benchmarks are run over a high number of nodes. Indeed, the benchmarks with
972 the same class, C, are executed on different numbers of nodes, so the
973 computation required for each iteration is divided by the number of computing
974 nodes. On the other hand, more communications are required when increasing the
975 number of nodes so the static energy increases linearly according to the
976 communication time and the dynamic power is less relevant in the overall energy
977 consumption. Therefore, reducing the frequency with Algorithm~\ref{HSA} is
978 less effective in reducing the overall energy savings. It can also be noticed
979 that for the benchmarks EP and SP that contain little or no communications, the
980 energy savings are not significantly affected by the high number of nodes. No
981 experiments were conducted using bigger classes than D, because they require a
982 lot of memory (more than 64GB) when being executed by the simulator on one
983 machine. The maximum distance between the normalized energy curve and the
984 normalized performance for each instance is also shown in the result tables. It
985 decrease in the same way as the energy saving percentage. The tables also show
986 that the performance degradation percentage is not significantly increased when
987 the number of computing nodes is increased because the computation times are
988 small when compared to the communication times.
994 \subfloat[Energy saving]{%
995 \includegraphics[width=.33\textwidth]{fig/energy}\label{fig:energy}}%
997 \subfloat[Performance degradation ]{%
998 \includegraphics[width=.33\textwidth]{fig/per_deg}\label{fig:per_deg}}
1000 \caption{The energy and performance for all NAS benchmarks running with a different number of nodes}
1003 Figures~\ref{fig:energy} and \ref{fig:per_deg} present the energy saving and
1004 performance degradation respectively for all the benchmarks according to the
1005 number of used nodes. As shown in the first plot, the energy saving percentages
1006 of the benchmarks MG, LU, BT and FT decrease linearly when the number of nodes
1007 increase. While for the EP and SP benchmarks, the energy saving percentage is
1008 not affected by the increase of the number of computing nodes, because in these
1009 benchmarks there are little or no communications. Finally, the energy saving of
1010 the GC benchmark significantly decrease when the number of nodes increase
1011 because this benchmark has more communications than the others. The second plot
1012 shows that the performance degradation percentages of most of the benchmarks
1013 decrease when they run on a big number of nodes because they spend more time
1014 communicating than computing, thus, scaling down the frequencies of some nodes
1015 has less effect on the performance.
1020 \subsection{The results for different power consumption scenarios}
1022 The results of the previous section were obtained while using processors that
1023 consume during computation an overall power which is 80\% composed of dynamic
1024 power and of 20\% of static power. In this section, these ratios are changed and
1025 two new power scenarios are considered in order to evaluate how the proposed
1026 algorithm adapts itself according to the static and dynamic power values. The
1027 two new power scenarios are the following:
1030 \item 70\% of dynamic power and 30\% of static power
1031 \item 90\% of dynamic power and 10\% of static power
1034 The NAS parallel benchmarks were executed again over processors that follow the
1035 new power scenarios. The class C of each benchmark was run over 8 or 9 nodes
1036 and the results are presented in Tables~\ref{table:res_s1} and
1037 \ref{table:res_s2}. These tables show that the energy saving percentage of the
1038 70\%-30\% scenario is smaller for all benchmarks compared to the energy saving
1039 of the 90\%-10\% scenario. Indeed, in the latter more dynamic power is consumed
1040 when nodes are running on their maximum frequencies, thus, scaling down the
1041 frequency of the nodes results in higher energy savings than in the 70\%-30\%
1042 scenario. On the other hand, the performance degradation percentage is smaller
1043 in the 70\%-30\% scenario compared to the 90\%-10\% scenario. This is due to the
1044 higher static power percentage in the first scenario which makes it more
1045 relevant in the overall consumed energy. Indeed, the static energy is related
1046 to the execution time and if the performance is degraded the amount of consumed
1047 static energy directly increases. Therefore, the proposed algorithm does not
1048 really significantly scale down much the frequencies of the nodes in order to
1049 limit the increase of the execution time and thus limiting the effect of the
1050 consumed static energy.
1052 Both new power scenarios are compared to the old one in
1053 Figure~\ref{fig:sen_comp}. It shows the average of the performance degradation, the
1054 energy saving and the distances for all NAS benchmarks of class C running on 8
1055 or 9 nodes. The comparison shows that the energy saving ratio is proportional
1056 to the dynamic power ratio: it is increased when applying the 90\%-10\% scenario
1057 because at maximum frequency the dynamic energy is the most relevant in the
1058 overall consumed energy and can be reduced by lowering the frequency of some
1059 processors. On the other hand, the energy saving decreases when the 70\%-30\%
1060 scenario is used because the dynamic energy is less relevant in the overall
1061 consumed energy and lowering the frequency does not return big energy savings.
1062 Moreover, the average of the performance degradation is decreased when using a
1063 higher ratio for static power (e.g. 70\%-30\% scenario and 80\%-20\%
1064 scenario). Since the proposed algorithm optimizes the energy consumption when
1065 using a higher ratio for dynamic power the algorithm selects bigger frequency
1066 scaling factors that result in more energy saving but less performance, for
1067 example see Figure~\ref{fig:scales_comp}. The opposite happens when using a
1068 higher ratio for static power, the algorithm proportionally selects smaller
1069 scaling values which result in less energy saving but also less performance
1074 \caption{The results of the 70\%-30\% power scenario}
1077 \begin{tabular}{|*{6}{r|}}
1079 Program & Energy & Energy & Performance & Distance \\
1080 name & consumption/J & saving\% & degradation\% & \\
1082 CG &4144.21 &22.42 &7.72 &14.70 \\
1084 MG &1133.23 &24.50 &5.34 &19.16 \\
1086 EP &6170.30 &16.19 &0.02 &16.17 \\
1088 LU &39477.28 &20.43 &0.07 &20.36 \\
1090 BT &26169.55 &25.34 &6.62 &18.71 \\
1092 SP &19620.09 &19.32 &3.66 &15.66 \\
1094 FT &6094.07 &23.17 &0.36 &22.81 \\
1097 \label{table:res_s1}
1103 \caption{The results of the 90\%-10\% power scenario}
1106 \begin{tabular}{|*{6}{r|}}
1108 Program & Energy & Energy & Performance & Distance \\
1109 name & consumption/J & saving\% & degradation\% & \\
1111 CG &2812.38 &36.36 &6.80 &29.56 \\
1113 MG &825.427 &38.35 &6.41 &31.94 \\
1115 EP &5281.62 &35.02 &2.68 &32.34 \\
1117 LU &31611.28 &39.15 &3.51 &35.64 \\
1119 BT &21296.46 &36.70 &6.60 &30.10 \\
1121 SP &15183.42 &35.19 &11.76 &23.43 \\
1123 FT &3856.54 &40.80 &5.67 &35.13 \\
1126 \label{table:res_s2}
1132 \subfloat[Comparison between the results on 8 nodes]{%
1133 \includegraphics[width=.33\textwidth]{fig/sen_comp}\label{fig:sen_comp}}%
1135 \subfloat[Comparison the selected frequency scaling factors of MG benchmark class C running on 8 nodes]{%
1136 \includegraphics[width=.33\textwidth]{fig/three_scenarios}\label{fig:scales_comp}}
1138 \caption{The comparison of the three power scenarios}
1144 \subsection{The comparison of the proposed scaling algorithm }
1145 \label{sec.compare_EDP}
1146 In this section, the scaling factors selection algorithm, called MaxDist,
1147 is compared to Spiliopoulos et al. algorithm \cite{Spiliopoulos_Green.governors.Adaptive.DVFS}, called EDP.
1148 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.
1149 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
1150 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.
1152 Both algorithms were applied to the parallel NAS benchmarks to compare their
1153 efficiency. Table~\ref{table:compare_EDP} presents the results of comparing the
1154 execution times and the energy consumption for both versions of the NAS
1155 benchmarks while running the class C of each benchmark over 8 or 9 heterogeneous
1156 nodes. The results show that our algorithm provides better energy savings than
1157 Spiliopoulos et al. algorithm, on average it results in 29.76\% energy saving
1158 while their algorithm returns just 25.75\%. The average of performance
1159 degradation percentage is approximately the same for both algorithms, about 4\%.
1162 For all benchmarks, our algorithm outperforms Spiliopoulos et al. algorithm in
1163 terms of energy and performance trade-off, see Figure~\ref{fig:compare_EDP},
1164 because it maximizes the distance between the energy saving and the performance
1165 degradation values while giving the same weight for both metrics.
1171 \caption{Comparing the proposed algorithm}
1173 \begin{tabular}{|*{7}{r|}}
1175 Program & \multicolumn{2}{c|}{Energy saving \%} & \multicolumn{2}{c|}{Perf. degradation \%} & \multicolumn{2}{c|}{Distance} \\ \cline{2-7}
1176 name & EDP & MaxDist & EDP & MaxDist & EDP & MaxDist \\ \hline
1177 CG & 27.58 & 31.25 & 5.82 & 7.12 & 21.76 & 24.13 \\ \hline
1178 MG & 29.49 & 33.78 & 3.74 & 6.41 & 25.75 & 27.37 \\ \hline
1179 LU & 19.55 & 28.33 & 0.0 & 0.01 & 19.55 & 28.22 \\ \hline
1180 EP & 28.40 & 27.04 & 4.29 & 0.49 & 24.11 & 26.55 \\ \hline
1181 BT & 27.68 & 32.32 & 6.45 & 7.87 & 21.23 & 24.43 \\ \hline
1182 SP & 20.52 & 24.73 & 5.21 & 2.78 & 15.31 & 21.95 \\ \hline
1183 FT & 27.03 & 31.02 & 2.75 & 2.54 & 24.28 & 28.48 \\ \hline
1186 \label{table:compare_EDP}
1195 \includegraphics[scale=0.5]{fig/compare_EDP.pdf}
1196 \caption{Trade-off comparison for NAS benchmarks class C}
1197 \label{fig:compare_EDP}
1201 \section{Conclusion}
1203 In this paper, a new online frequency selecting algorithm has been presented. It
1204 selects the best possible vector of frequency scaling factors that gives the
1205 maximum distance (optimal trade-off) between the predicted energy and the
1206 predicted performance curves for a heterogeneous platform. This algorithm uses a
1207 new energy model for measuring and predicting the energy of distributed
1208 iterative applications running over heterogeneous platforms. To evaluate the
1209 proposed method, it was applied on the NAS parallel benchmarks and executed over
1210 a heterogeneous platform simulated by SimGrid. The results of the experiments
1211 showed that the algorithm reduces up to 35\% the energy consumption of a message
1212 passing iterative method while limiting the degradation of the performance. The
1213 algorithm also selects different scaling factors according to the percentage of
1214 the computing and communication times, and according to the values of the static
1215 and dynamic powers of the CPUs. Finally, the algorithm was compared to
1216 Spiliopoulos et al. algorithm and the results showed that it outperforms their
1217 algorithm in terms of energy-time trade-off.
1219 In the near future, this method will be applied to real heterogeneous platforms
1220 to evaluate its performance in a real study case. It would also be interesting
1221 to evaluate its scalability over large scale heterogeneous platforms and measure
1222 the energy consumption reduction it can produce. Afterward, we would like to
1223 develop a similar method that is adapted to asynchronous iterative applications
1224 where each task does not wait for other tasks to finish their works. The
1225 development of such a method might require a new energy model because the number
1226 of iterations is not known in advance and depends on the global convergence of
1227 the iterative system.
1229 \section*{Acknowledgment}
1231 This work has been partially supported by the Labex
1232 ACTION project (contract “ANR-11-LABX-01-01”). As a PhD student,
1233 Mr. Ahmed Fanfakh, would like to thank the University of
1234 Babylon (Iraq) for supporting his work.
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1251 %%% ispell-local-dictionary: "american"
1254 % LocalWords: Fanfakh Charr FIXME Tianhe DVFS HPC NAS NPB SMPI Rauber's Rauber
1255 % LocalWords: CMOS EPSA Franche Comté Tflop Rünger IUT Maréchal Juin cedex GPU
1256 % LocalWords: de badri muslim MPI TcpOld TcmOld dNew dOld cp Sopt Tcp Tcm Ps
1257 % LocalWords: Scp Fmax Fdiff SimGrid GFlops Xeon EP BT GPUs CPUs AMD
1258 % LocalWords: Spiliopoulos scalability