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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 ... 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
156 same goal. Reducing the frequency of a processor lowers its number of FLOPS and
157 might degrade the performance of the application running on that processor,
158 especially if it is compute bound. Therefore selecting the appropriate frequency
159 for a 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 as
163 ~\cite{Hao_Learning.based.DVFS,Spiliopoulos_Green.governors.Adaptive.DVFS}. Others
164 used offline methods that might need to run the application and profile it
165 before selecting the new frequency, such as
166 ~\cite{Rountree_Bounding.energy.consumption.in.MPI,Cochran_Pack_and_Cap_Adaptive_DVFS}. The
167 methods could be heuristics, exact or brute force methods that satisfy varied
168 objectives such as energy reduction or performance. They also could be adapted
169 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, ...
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 executed on the GPUs and the rest are executed
183 on the CPUs. Luley et al.
184 ~\cite{Luley_Energy.efficiency.evaluation.and.benchmarking}, proposed a heterogeneous
185 cluster composed of Intel Xeon CPUs and NVIDIA GPUs. Their main goal was to maximize the
186 energy efficiency of the platform during computation by maximizing the number of FLOPS per watt generated.
187 In~\cite{KaiMa_Holistic.Approach.to.Energy.Efficiency.in.GPU-CPU}, Kai Ma et al. developed a scheduling
188 algorithm that distributes workloads proportional to the computing power of the nodes which could be a GPU or a CPU. All the tasks must be completed at the same time.
189 In~\cite{Rong_Effects.of.DVFS.on.K20.GPU}, Rong et al. showed that
190 a heterogeneous (GPUs and CPUs) cluster that enables DVFS gave better energy and performance
191 efficiency than other clusters only composed of CPUs.
193 The work presented in this paper concerns the second type of platform, with heterogeneous CPUs.
194 Many methods were conceived to reduce the energy consumption of this type of platform. Naveen et al.~\cite{Naveen_Power.Efficient.Resource.Scaling}
195 developed a method that minimizes the value of $energy\cdot delay^2$ (the delay is the sum of slack times that happen during synchronous communications) by dynamically assigning new frequencies to the CPUs of the heterogeneous cluster. Lizhe et al.~\cite{Lizhe_Energy.aware.parallel.task.scheduling} proposed
196 an algorithm that divides the executed tasks into two types: the critical and
197 non critical tasks. The algorithm scales down the frequency of non critical tasks proportionally to their slack and communication times while limiting the performance degradation percentage to less than 10\%. In~\cite{Joshi_Blackbox.prediction.of.impact.of.DVFS}, they developed
198 a heterogeneous cluster composed of two types
199 of Intel and AMD processors. They use a gradient method to predict the impact of DVFS operations on performance.
200 In~\cite{Shelepov_Scheduling.on.Heterogeneous.Multicore} and \cite{Li_Minimizing.Energy.Consumption.for.Frame.Based.Tasks},
201 the best frequencies for a specified heterogeneous cluster are selected offline using some
202 heuristic. Chen et al.~\cite{Chen_DVFS.under.quality.of.service.requirements} used a greedy dynamic programming approach to
203 minimize the power consumption of heterogeneous servers while respecting given time constraints. This approach
204 had considerable overhead.
205 In contrast to the above described papers, this paper presents the following contributions :
207 \item two new energy and performance models for message passing iterative synchronous applications running over
208 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.
210 \item a new online frequency selecting algorithm for heterogeneous platforms. The algorithm has a very small
211 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.
215 \section{The performance and energy consumption measurements on heterogeneous architecture}
220 \subsection{The execution time of message passing distributed
221 iterative applications on a heterogeneous platform}
223 In this paper, we are interested in reducing the energy consumption of message
224 passing distributed iterative synchronous applications running over
225 heterogeneous platforms. A heterogeneous platform is defined as a collection of
226 heterogeneous computing nodes interconnected via a high speed homogeneous
227 network. Therefore, each node has different characteristics such as computing
228 power (FLOPS), energy consumption, CPU's frequency range, \dots{} but they all
229 have the same network bandwidth and latency.
231 The overall execution time of a distributed iterative synchronous application
232 over a heterogeneous platform consists of the sum of the computation time and
233 the communication time for every iteration on a node. However, due to the
234 heterogeneous computation power of the computing nodes, slack times might occur
235 when fast nodes have to wait, during synchronous communications, for the slower
236 nodes to finish their computations (see Figure~(\ref{fig:heter})).
237 Therefore, the overall execution time of the program is the execution time of the slowest
238 task which has the highest computation time and no slack time.
242 \includegraphics[scale=0.6]{fig/commtasks}
243 \caption{Parallel tasks on a heterogeneous platform}
247 Dynamic Voltage and Frequency Scaling (DVFS) is a process, implemented in
248 modern processors, that reduces the energy consumption of a CPU by scaling
249 down its voltage and frequency. Since DVFS lowers the frequency of a CPU
250 and consequently its computing power, the execution time of a program running
251 over that scaled down processor might increase, especially if the program is
252 compute bound. The frequency reduction process can be expressed by the scaling
253 factor S which is the ratio between the maximum and the new frequency of a CPU
257 S = \frac{F_\textit{max}}{F_\textit{new}}
259 The execution time of a compute bound sequential program is linearly proportional
260 to the frequency scaling factor $S$. On the other hand, message passing
261 distributed applications consist of two parts: computation and communication.
262 The execution time of the computation part is linearly proportional to the
263 frequency scaling factor $S$ but the communication time is not affected by the
264 scaling factor because the processors involved remain idle during the
265 communications~\cite{Freeh_Exploring.the.Energy.Time.Tradeoff}.
266 The communication time for a task is the summation of periods of
267 time that begin with an MPI call for sending or receiving a message
268 until the message is synchronously sent or received.
270 Since in a heterogeneous platform each node has different characteristics,
271 especially different frequency gears, when applying DVFS operations on these
272 nodes, they may get different scaling factors represented by a scaling vector:
273 $(S_1, S_2,\dots, S_N)$ where $S_i$ is the scaling factor of processor $i$. To
274 be able to predict the execution time of message passing synchronous iterative
275 applications running over a heterogeneous platform, for different vectors of
276 scaling factors, the communication time and the computation time for all the
277 tasks must be measured during the first iteration before applying any DVFS
278 operation. Then the execution time for one iteration of the application with any
279 vector of scaling factors can be predicted using (\ref{eq:perf}).
282 \textit T_\textit{new} =
283 \max_{i=1,2,\dots,N} ({TcpOld_{i}} \cdot S_{i}) + MinTcm
288 MinTcm = \min_{i=1,2,\dots,N} (Tcm_i)
290 where $TcpOld_i$ is the computation time of processor $i$ during the first
291 iteration and $MinTcm$ is the communication time of the slowest processor from
292 the first iteration. The model computes the maximum computation time with
293 scaling factor from each node added to the communication time of the slowest
294 node. It means only the communication time without any slack time is taken into
295 account. Therefore, the execution time of the iterative application is equal to
296 the execution time of one iteration as in (\ref{eq:perf}) multiplied by the
297 number of iterations of that application.
299 This prediction model is developed from the model to predict the execution time
300 of message passing distributed applications for homogeneous
301 architectures~\cite{Our_first_paper}. The execution time prediction model is
302 used in the method to optimize both the energy consumption and the performance of
303 iterative methods, which is presented in the following sections.
306 \subsection{Energy model for heterogeneous platform}
307 Many researchers~\cite{Malkowski_energy.efficient.high.performance.computing,
308 Rauber_Analytical.Modeling.for.Energy,Zhuo_Energy.efficient.Dynamic.Task.Scheduling,
309 Rizvandi_Some.Observations.on.Optimal.Frequency} divide the power consumed by a processor into
310 two power metrics: the static and the dynamic power. While the first one is
311 consumed as long as the computing unit is turned on, the latter is only consumed during
312 computation times. The dynamic power $Pd$ is related to the switching
313 activity $\alpha$, load capacitance $C_L$, the supply voltage $V$ and
314 operational frequency $F$, as shown in (\ref{eq:pd}).
317 Pd = \alpha \cdot C_L \cdot V^2 \cdot F
319 The static power $Ps$ captures the leakage power as follows:
322 Ps = V \cdot N_{trans} \cdot K_{design} \cdot I_{leak}
324 where V is the supply voltage, $N_{trans}$ is the number of transistors,
325 $K_{design}$ is a design dependent parameter and $I_{leak}$ is a
326 technology dependent parameter. The energy consumed by an individual processor
327 to execute a given program can be computed as:
330 E_\textit{ind} = Pd \cdot Tcp + Ps \cdot T
332 where $T$ is the execution time of the program, $Tcp$ is the computation
333 time and $Tcp \le T$. $Tcp$ may be equal to $T$ if there is no
334 communication and no slack time.
336 The main objective of DVFS operation is to reduce the overall energy consumption~\cite{Le_DVFS.Laws.of.Diminishing.Returns}.
337 The operational frequency $F$ depends linearly on the supply voltage $V$, i.e., $V = \beta \cdot F$ with some
338 constant $\beta$.~This equation is used to study the change of the dynamic
339 voltage with respect to various frequency values in~\cite{Rauber_Analytical.Modeling.for.Energy}. The reduction
340 process of the frequency can be expressed by the scaling factor $S$ which is the
341 ratio between the maximum and the new frequency as in (\ref{eq:s}).
342 The CPU governors are power schemes supplied by the operating
343 system's kernel to lower a core's frequency. The new frequency
344 $F_{new}$ from (\ref{eq:s}) can be calculated as follows:
347 F_\textit{new} = S^{-1} \cdot F_\textit{max}
349 Replacing $F_{new}$ in (\ref{eq:pd}) as in (\ref{eq:fnew}) gives the following
350 equation for dynamic power consumption:
353 {P}_\textit{dNew} = \alpha \cdot C_L \cdot V^2 \cdot F_{new} = \alpha \cdot C_L \cdot \beta^2 \cdot F_{new}^3 \\
354 {} = \alpha \cdot C_L \cdot V^2 \cdot F_{max} \cdot S^{-3} = P_{dOld} \cdot S^{-3}
356 where $ {P}_\textit{dNew}$ and $P_{dOld}$ are the dynamic power consumed with the
357 new frequency and the maximum frequency respectively.
359 According to (\ref{eq:pdnew}) the dynamic power is reduced by a factor of $S^{-3}$ when
360 reducing the frequency by a factor of $S$~\cite{Rauber_Analytical.Modeling.for.Energy}. Since the FLOPS of a CPU is proportional
361 to the frequency of a CPU, the computation time is increased proportionally to $S$.
362 The new dynamic energy is the dynamic power multiplied by the new time of computation
363 and is given by the following equation:
366 E_\textit{dNew} = P_{dOld} \cdot S^{-3} \cdot (Tcp \cdot S)= S^{-2}\cdot P_{dOld} \cdot Tcp
368 The static power is related to the power leakage of the CPU and is consumed during computation
369 and even when idle. As in~\cite{Rauber_Analytical.Modeling.for.Energy,Zhuo_Energy.efficient.Dynamic.Task.Scheduling},
370 the static power of a processor is considered as constant
371 during idle and computation periods, and for all its available frequencies.
372 The static energy is the static power multiplied by the execution time of the program.
373 According to the execution time model in (\ref{eq:perf}), the execution time of the program
374 is the sum of the computation and the communication times. The computation time is linearly related
375 to the frequency scaling factor, while this scaling factor does not affect the communication time.
376 The static energy of a processor after scaling its frequency is computed as follows:
379 E_\textit{s} = Ps \cdot (Tcp \cdot S + Tcm)
382 In the considered heterogeneous platform, each processor $i$ might have
383 different dynamic and static powers, noted as $Pd_{i}$ and $Ps_{i}$
384 respectively. Therefore, even if the distributed message passing iterative
385 application is load balanced, the computation time of each CPU $i$ noted
386 $Tcp_{i}$ might be different and different frequency scaling factors might be
387 computed in order to decrease the overall energy consumption of the application
388 and reduce slack times. The communication time of a processor $i$ is noted as
389 $Tcm_{i}$ and could contain slack times when communicating with slower
390 nodes, see figure(\ref{fig:heter}). Therefore, all nodes do not have equal
391 communication times. While the dynamic energy is computed according to the
392 frequency scaling factor and the dynamic power of each node as in
393 (\ref{eq:Edyn}), the static energy is computed as the sum of the execution time
394 of one iteration multiplied by the static power of each processor. The overall
395 energy consumption of a message passing distributed application executed over a
396 heterogeneous platform during one iteration is the summation of all dynamic and
397 static energies for each processor. It is computed as follows:
400 E = \sum_{i=1}^{N} {(S_i^{-2} \cdot Pd_{i} \cdot Tcp_i)} + {} \\
401 \sum_{i=1}^{N} (Ps_{i} \cdot (\max_{i=1,2,\dots,N} (Tcp_i \cdot S_{i}) +
405 Reducing the frequencies of the processors according to the vector of
406 scaling factors $(S_1, S_2,\dots, S_N)$ may degrade the performance of the
407 application and thus, increase the static energy because the execution time is
408 increased~\cite{Kim_Leakage.Current.Moore.Law}. The overall energy consumption for the iterative
409 application can be measured by measuring the energy consumption for one iteration as in (\ref{eq:energy})
410 multiplied by the number of iterations of that application.
413 \section{Optimization of both energy consumption and performance}
416 Using the lowest frequency for each processor does not necessarily give the most
417 energy efficient execution of an application. Indeed, even though the dynamic
418 power is reduced while scaling down the frequency of a processor, its
419 computation power is proportionally decreased. Hence, the execution time might
420 be drastically increased and during that time, dynamic and static powers are
421 being consumed. Therefore, it might cancel any gains achieved by scaling down
422 the frequency of all nodes to the minimum and the overall energy consumption of
423 the application might not be the optimal one. It is not trivial to select the
424 appropriate frequency scaling factor for each processor while considering the
425 characteristics of each processor (computation power, range of frequencies,
426 dynamic and static powers) and the task executed (computation/communication
427 ratio). The aim being to reduce the overall energy consumption and to avoid
428 increasing significantly the execution time. In our previous
429 work~\cite{Our_first_paper}, we proposed a method that selects the optimal
430 frequency scaling factor for a homogeneous cluster executing a message passing
431 iterative synchronous application while giving the best trade-off between the
432 energy consumption and the performance for such applications. In this work we
433 are interested in heterogeneous clusters as described above. Due to the
434 heterogeneity of the processors, a vector of scaling factors should
435 be selected and it must give the best trade-off between energy consumption and
438 The relation between the energy consumption and the execution time for an
439 application is complex and nonlinear, Thus, unlike the relation between the
440 execution time and the scaling factor, the relation between the energy and the
441 frequency scaling factors is nonlinear, for more details refer
442 to~\cite{Freeh_Exploring.the.Energy.Time.Tradeoff}. Moreover, these relations
443 are not measured using the same metric. To solve this problem, the execution
444 time is normalized by computing the ratio between the new execution time (after
445 scaling down the frequencies of some processors) and the initial one (with
446 maximum frequency for all nodes) as follows:
449 P_\textit{Norm} = \frac{T_\textit{New}}{T_\textit{Old}}\\
450 {} = \frac{ \max_{i=1,2,\dots,N} (Tcp_{i} \cdot S_{i}) +MinTcm}
451 {\max_{i=1,2,\dots,N}{(Tcp_i+Tcm_i)}}
455 In the same way, the energy is normalized by computing the ratio between the consumed energy
456 while scaling down the frequency and the consumed energy with maximum frequency for all nodes:
459 E_\textit{Norm} = \frac{E_\textit{Reduced}}{E_\textit{Original}} \\
460 {} = \frac{ \sum_{i=1}^{N}{(S_i^{-2} \cdot Pd_i \cdot Tcp_i)} +
461 \sum_{i=1}^{N} {(Ps_i \cdot T_{New})}}{\sum_{i=1}^{N}{( Pd_i \cdot Tcp_i)} +
462 \sum_{i=1}^{N} {(Ps_i \cdot T_{Old})}}
464 Where $E_\textit{Reduced}$ and $E_\textit{Original}$ are computed using (\ref{eq:energy}) and
465 $T_{New}$ and $T_{Old}$ are computed as in (\ref{eq:pnorm}).
468 goal is to optimize the energy and execution time at the same time, the normalized
469 energy and execution time curves are not in the same direction. According
470 to the equations~(\ref{eq:pnorm}) and (\ref{eq:enorm}), the vector of frequency
471 scaling factors $S_1,S_2,\dots,S_N$ reduce both the energy and the execution
472 time simultaneously. But the main objective is to produce maximum energy
473 reduction with minimum execution time reduction.
475 This problem can be solved by making the optimization process for energy and
476 execution time following the same direction. Therefore, the equation of the
477 normalized execution time is inverted which gives the normalized performance equation, as follows:
480 P_\textit{Norm} = \frac{T_\textit{Old}}{T_\textit{New}}\\
481 = \frac{\max_{i=1,2,\dots,N}{(Tcp_i+Tcm_i)}}
482 { \max_{i=1,2,\dots,N} (Tcp_{i} \cdot S_{i}) + MinTcm}
488 \subfloat[Homogeneous platform]{%
489 \includegraphics[width=.33\textwidth]{fig/homo}\label{fig:r1}}%
492 \subfloat[Heterogeneous platform]{%
493 \includegraphics[width=.33\textwidth]{fig/heter}\label{fig:r2}}
495 \caption{The energy and performance relation}
498 Then, the objective function can be modeled in order to find the maximum distance
499 between the energy curve (\ref{eq:enorm}) and the performance
500 curve (\ref{eq:pnorm_inv}) over all available sets of scaling factors. This
501 represents the minimum energy consumption with minimum execution time (maximum
502 performance) at the same time, see figure~(\ref{fig:r1}) or figure~(\ref{fig:r2}). Then the objective
503 function has the following form:
507 \max_{i=1,\dots F, j=1,\dots,N}
508 (\overbrace{P_\textit{Norm}(S_{ij})}^{\text{Maximize}} -
509 \overbrace{E_\textit{Norm}(S_{ij})}^{\text{Minimize}} )
511 where $N$ is the number of nodes and $F$ is the number of available frequencies for each node.
512 Then, the optimal set of scaling factors that satisfies (\ref{eq:max}) can be selected.
513 The objective function can work with any energy model or any power values for each node
514 (static and dynamic powers). However, the most important energy reduction gain can be achieved when
515 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}.
517 \section{The scaling factors selection algorithm for heterogeneous platforms }
520 \subsection{The algorithm details}
521 In this section, algorithm \ref{HSA} is presented. It selects the frequency scaling factors
522 vector that gives the best trade-off between minimizing the energy consumption and maximizing
523 the performance of a message passing synchronous iterative application executed on a heterogeneous
524 platform. It works online during the execution time of the iterative message passing program.
525 It uses information gathered during the first iteration such as the computation time and the
526 communication time in one iteration for each node. The algorithm is executed after the first
527 iteration and returns a vector of optimal frequency scaling factors that satisfies the objective
528 function (\ref{eq:max}). The program applies DVFS operations to change the frequencies of the CPUs
529 according to the computed scaling factors. This algorithm is called just once during the execution
530 of the program. Algorithm~(\ref{dvfs}) shows where and when the proposed scaling algorithm is called
531 in the iterative MPI program.
533 The nodes in a heterogeneous platform have different computing powers, thus while executing message
534 passing iterative synchronous applications, fast nodes have to wait for the slower ones to finish their
535 computations before being able to synchronously communicate with them as in figure (\ref{fig:heter}).
536 These periods are called idle or slack times.
537 The algorithm takes into account this problem and tries to reduce these slack times when selecting the
538 frequency scaling factors vector. At first, it selects initial frequency scaling factors that increase
539 the execution times of fast nodes and minimize the differences between the computation times of
540 fast and slow nodes. The value of the initial frequency scaling factor for each node is inversely
541 proportional to its computation time that was gathered from the first iteration. These initial frequency
542 scaling factors are computed as a ratio between the computation time of the slowest node and the
543 computation time of the node $i$ as follows:
546 Scp_{i} = \frac{\max_{i=1,2,\dots,N}(Tcp_i)}{Tcp_i}
548 Using the initial frequency scaling factors computed in (\ref{eq:Scp}), the algorithm computes
549 the initial frequencies for all nodes as a ratio between the maximum frequency of node $i$
550 and the computation scaling factor $Scp_i$ as follows:
553 F_{i} = \frac{Fmax_i}{Scp_i},~{i=1,2,\cdots,N}
555 If the computed initial frequency for a node is not available in the gears of
556 that node, it is replaced by the nearest available frequency. In figure
557 (\ref{fig:st_freq}), the nodes are sorted by their computing power in ascending
558 order and the frequencies of the faster nodes are scaled down according to the
559 computed initial frequency scaling factors. The resulting new frequencies are
560 colored in blue in figure (\ref{fig:st_freq}). This set of frequencies can be
561 considered as a higher bound for the search space of the optimal vector of
562 frequencies because selecting frequency scaling factors higher than the higher
563 bound will not improve the performance of the application and it will increase
564 its overall energy consumption. Therefore the algorithm that selects the
565 frequency scaling factors starts the search method from these initial
566 frequencies and takes a downward search direction toward lower frequencies. The
567 algorithm iterates on all left frequencies, from the higher bound until all
568 nodes reach their minimum frequencies, to compute their overall energy
569 consumption and performance, and select the optimal frequency scaling factors
570 vector. At each iteration the algorithm determines the slowest node according to
571 the equation (\ref{eq:perf}) and keeps its frequency unchanged, while it lowers
572 the frequency of all other nodes by one gear. The new overall energy
573 consumption and execution time are computed according to the new scaling
574 factors. The optimal set of frequency scaling factors is the set that gives the
575 highest distance according to the objective function (\ref{eq:max}).
577 Figures~\ref{fig:r1} and \ref{fig:r2} illustrate the normalized performance and
578 consumed energy for an application running on a homogeneous platform and a
579 heterogeneous platform respectively while increasing the scaling factors. It can
580 be noticed that in a homogeneous platform the search for the optimal scaling
581 factor should start from the maximum frequency because the performance and the
582 consumed energy decrease from the beginning of the plot. On the other hand,
583 in the heterogeneous platform the performance is maintained at the beginning of
584 the plot even if the frequencies of the faster nodes decrease until the
585 computing power of scaled down nodes are lower than the slowest node. In other
586 words, until they reach the higher bound. It can also be noticed that the higher
587 the difference between the faster nodes and the slower nodes is, the bigger the
588 maximum distance between the energy curve and the performance curve is while
589 the scaling factors are varying which results in bigger energy savings.
592 \includegraphics[scale=0.5]{fig/start_freq}
593 \caption{Selecting the initial frequencies}
601 \begin{algorithmic}[1]
605 \item[$Tcp_i$] array of all computation times for all nodes during one iteration and with highest frequency.
606 \item[$Tcm_i$] array of all communication times for all nodes during one iteration and with highest frequency.
607 \item[$Fmax_i$] array of the maximum frequencies for all nodes.
608 \item[$Pd_i$] array of the dynamic powers for all nodes.
609 \item[$Ps_i$] array of the static powers for all nodes.
610 \item[$Fdiff_i$] array of the difference between two successive frequencies for all nodes.
612 \Ensure $Sopt_1,Sopt_2 \dots, Sopt_N$ is a vector of optimal scaling factors
614 \State $ Scp_i \gets \frac{\max_{i=1,2,\dots,N}(Tcp_i)}{Tcp_i} $
615 \State $F_{i} \gets \frac{Fmax_i}{Scp_i},~{i=1,2,\cdots,N}$
616 \State Round the computed initial frequencies $F_i$ to the closest one available in each node.
617 \If{(not the first frequency)}
618 \State $F_i \gets F_i+Fdiff_i,~i=1,\dots,N.$
620 \State $T_\textit{Old} \gets max_{~i=1,\dots,N } (Tcp_i+Tcm_i)$
621 \State $E_\textit{Original} \gets \sum_{i=1}^{N}{( Pd_i \cdot Tcp_i)} +\sum_{i=1}^{N} {(Ps_i \cdot T_{Old})}$
622 \State $Sopt_{i} \gets 1,~i=1,\dots,N. $
623 \State $Dist \gets 0 $
624 \While {(all nodes not reach their minimum frequency)}
625 \If{(not the last freq. \textbf{and} not the slowest node)}
626 \State $F_i \gets F_i - Fdiff_i,~i=1,\dots,N.$
627 \State $S_i \gets \frac{Fmax_i}{F_i},~i=1,\dots,N.$
629 \State $T_{New} \gets max_\textit{~i=1,\dots,N} (Tcp_{i} \cdot S_{i}) + MinTcm $
630 \State $E_\textit{Reduced} \gets \sum_{i=1}^{N}{(S_i^{-2} \cdot Pd_i \cdot Tcp_i)} + $ \hspace*{43 mm}
631 $\sum_{i=1}^{N} {(Ps_i \cdot T_{New})} $
632 \State $ P_\textit{Norm} \gets \frac{T_\textit{Old}}{T_\textit{New}}$
633 \State $E_\textit{Norm}\gets \frac{E_\textit{Reduced}}{E_\textit{Original}}$
634 \If{$(\Pnorm - \Enorm > \Dist)$}
635 \State $Sopt_{i} \gets S_{i},~i=1,\dots,N. $
636 \State $\Dist \gets \Pnorm - \Enorm$
639 \State Return $Sopt_1,Sopt_2,\dots,Sopt_N$
641 \caption{frequency scaling factors selection algorithm}
646 \begin{algorithmic}[1]
648 \For {$k=1$ to \textit{some iterations}}
649 \State Computations section.
650 \State Communications section.
652 \State Gather all times of computation and\newline\hspace*{3em}%
653 communication from each node.
654 \State Call algorithm \ref{HSA}.
655 \State Compute the new frequencies from the\newline\hspace*{3em}%
656 returned optimal scaling factors.
657 \State Set the new frequencies to nodes.
661 \caption{DVFS algorithm}
665 \subsection{The evaluation of the proposed algorithm}
666 \label{sec.verif.algo}
667 The precision of the proposed algorithm mainly depends on the execution time
668 prediction model defined in (\ref{eq:perf}) and the energy model computed by
669 (\ref{eq:energy}). The energy model is also significantly dependent on the
670 execution time model because the static energy is linearly related to the
671 execution time and the dynamic energy is related to the computation time. So,
672 all the works presented in this paper are based on the execution time model. To
673 verify this model, the predicted execution time was compared to the real
674 execution time over SimGrid/SMPI simulator,
675 v3.10~\cite{casanova+giersch+legrand+al.2014.versatile}, for all the NAS
676 parallel benchmarks NPB v3.3 \cite{NAS.Parallel.Benchmarks}, running class B on
677 8 or 9 nodes. The comparison showed that the proposed execution time model is
678 very precise, the maximum normalized difference between the predicted execution
679 time and the real execution time is equal to 0.03 for all the NAS benchmarks.
681 Since the proposed algorithm is not an exact method it does not test all the possible solutions (vectors of scaling factors)
682 in the search space. To prove its efficiency, it was compared on small instances to a brute force search algorithm
683 that tests all the possible solutions. The brute force algorithm was applied to different NAS benchmarks classes with
684 different number of nodes. The solutions returned by the brute force algorithm and the proposed algorithm were identical
685 and the proposed algorithm was on average 10 times faster than the brute force algorithm. It has a small execution time:
686 for a heterogeneous cluster composed of four different types of nodes having the characteristics presented in
687 table~\ref{table:platform}, it takes on average \np[ms]{0.04} for 4 nodes and \np[ms]{0.15} on average for 144 nodes
688 to compute the best scaling factors vector. The algorithm complexity is $O(F\cdot (N \cdot4) )$, where $F$ is the number
689 of iterations and $N$ is the number of computing nodes. The algorithm needs from 12 to 20 iterations to select the best
690 vector of frequency scaling factors that gives the results of the next sections.
692 \section{Experimental results}
694 To evaluate the efficiency and the overall energy consumption reduction of
695 algorithm~\ref{HSA}, it was applied to the NAS parallel benchmarks NPB v3.3. The
696 experiments were executed on the simulator SimGrid/SMPI which offers easy tools
697 to create a heterogeneous platform and run message passing applications over it.
698 The heterogeneous platform that was used in the experiments, had one core per
699 node because just one process was executed per node. The heterogeneous platform
700 was composed of four types of nodes. Each type of nodes had different
701 characteristics such as the maximum CPU frequency, the number of available
702 frequencies and the computational power, see Table \ref{table:platform}. The
703 characteristics of these different types of nodes are inspired from the
704 specifications of real Intel processors. The heterogeneous platform had up to
705 144 nodes and had nodes from the four types in equal proportions, for example if
706 a benchmark was executed on 8 nodes, 2 nodes from each type were used. Since the
707 constructors of CPUs do not specify the dynamic and the static power of their
708 CPUs, for each type of node they were chosen proportionally to its computing
709 power (FLOPS). In the initial heterogeneous platform, while computing with
710 highest frequency, each node consumed an amount of power proportional to its
711 computing power (which corresponds to 80\% of its dynamic power and the
712 remaining 20\% to the static power), the same assumption was made in
713 \cite{Our_first_paper,Rauber_Analytical.Modeling.for.Energy}. Finally, These
714 nodes were connected via an Ethernet network with 1 Gbit/s bandwidth.
718 \caption{Heterogeneous nodes characteristics}
721 \begin{tabular}{|*{7}{l|}}
723 Node &Simulated & Max & Min & Diff. & Dynamic & Static \\
724 type &GFLOPS & Freq. & Freq. & Freq. & power & power \\
725 & & GHz & GHz &GHz & & \\
727 1 &40 & 2.5 & 1.2 & 0.1 & 20~W &4~W \\
730 2 &50 & 2.66 & 1.6 & 0.133 & 25~W &5~W \\
733 3 &60 & 2.9 & 1.2 & 0.1 & 30~W &6~W \\
736 4 &70 & 3.4 & 1.6 & 0.133 & 35~W &7~W \\
740 \label{table:platform}
744 %\subsection{Performance prediction verification}
747 \subsection{The experimental results of the scaling algorithm}
751 The proposed algorithm was applied to the seven parallel NAS benchmarks (EP, CG,
752 MG, FT, BT, LU and SP) and the benchmarks were executed with the three classes:
753 A, B and C. However, due to the lack of space in this paper, only the results of
754 the biggest class, C, are presented while being run on different number of
755 nodes, ranging from 4 to 128 or 144 nodes depending on the benchmark being
756 executed. Indeed, the benchmarks CG, MG, LU, EP and FT had to be executed on $1,
757 2, 4, 8, 16, 32, 64, 128$ nodes. The other benchmarks such as BT and SP had to
758 be executed on $1, 4, 9, 16, 36, 64, 144$ nodes.
763 \caption{Running NAS benchmarks on 4 nodes }
766 \begin{tabular}{|*{7}{r|}}
768 Program & Execution & Energy & Energy & Performance & Distance \\
769 name & time/s & consumption/J & saving\% & degradation\% & \\
771 CG & 64.64 & 3560.39 &34.16 &6.72 &27.44 \\
773 MG & 18.89 & 1074.87 &35.37 &4.34 &31.03 \\
775 EP &79.73 &5521.04 &26.83 &3.04 &23.79 \\
777 LU &308.65 &21126.00 &34.00 &6.16 &27.84 \\
779 BT &360.12 &21505.55 &35.36 &8.49 &26.87 \\
781 SP &234.24 &13572.16 &35.22 &5.70 &29.52 \\
783 FT &81.58 &4151.48 &35.58 &0.99 &34.59 \\
791 \caption{Running NAS benchmarks on 8 and 9 nodes }
794 \begin{tabular}{|*{7}{r|}}
796 Program & Execution & Energy & Energy & Performance & Distance \\
797 name & time/s & consumption/J & saving\% & degradation\% & \\
799 CG &36.11 &3263.49 &31.25 &7.12 &24.13 \\
801 MG &8.99 &953.39 &33.78 &6.41 &27.37 \\
803 EP &40.39 &5652.81 &27.04 &0.49 &26.55 \\
805 LU &218.79 &36149.77 &28.23 &0.01 &28.22 \\
807 BT &166.89 &23207.42 &32.32 &7.89 &24.43 \\
809 SP &104.73 &18414.62 &24.73 &2.78 &21.95 \\
811 FT &51.10 &4913.26 &31.02 &2.54 &28.48 \\
819 \caption{Running NAS benchmarks on 16 nodes }
822 \begin{tabular}{|*{7}{r|}}
824 Program & Execution & Energy & Energy & Performance & Distance \\
825 name & time/s & consumption/J & saving\% & degradation\% & \\
827 CG &31.74 &4373.90 &26.29 &9.57 &16.72 \\
829 MG &5.71 &1076.19 &32.49 &6.05 &26.44 \\
831 EP &20.11 &5638.49 &26.85 &0.56 &26.29 \\
833 LU &144.13 &42529.06 &28.80 &6.56 &22.24 \\
835 BT &97.29 &22813.86 &34.95 &5.80 &29.15 \\
837 SP &66.49 &20821.67 &22.49 &3.82 &18.67 \\
839 FT &37.01 &5505.60 &31.59 &6.48 &25.11 \\
842 \label{table:res_16n}
847 \caption{Running NAS benchmarks on 32 and 36 nodes }
850 \begin{tabular}{|*{7}{r|}}
852 Program & Execution & Energy & Energy & Performance & Distance \\
853 name & time/s & consumption/J & saving\% & degradation\% & \\
855 CG &32.35 &6704.21 &16.15 &5.30 &10.85 \\
857 MG &4.30 &1355.58 &28.93 &8.85 &20.08 \\
859 EP &9.96 &5519.68 &26.98 &0.02 &26.96 \\
861 LU &99.93 &67463.43 &23.60 &2.45 &21.15 \\
863 BT &48.61 &23796.97 &34.62 &5.83 &28.79 \\
865 SP &46.01 &27007.43 &22.72 &3.45 &19.27 \\
867 FT &28.06 &7142.69 &23.09 &2.90 &20.19 \\
870 \label{table:res_32n}
875 \caption{Running NAS benchmarks on 64 nodes }
878 \begin{tabular}{|*{7}{r|}}
880 Program & Execution & Energy & Energy & Performance & Distance \\
881 name & time/s & consumption/J & saving\% & degradation\% & \\
883 CG &46.65 &17521.83 &8.13 &1.68 &6.45 \\
885 MG &3.27 &1534.70 &29.27 &14.35 &14.92 \\
887 EP &5.05 &5471.1084 &27.12 &3.11 &24.01 \\
889 LU &73.92 &101339.16 &21.96 &3.67 &18.29 \\
891 BT &39.99 &27166.71 &32.02 &12.28 &19.74 \\
893 SP &52.00 &49099.28 &24.84 &0.03 &24.81 \\
895 FT &25.97 &10416.82 &20.15 &4.87 &15.28 \\
898 \label{table:res_64n}
903 \caption{Running NAS benchmarks on 128 and 144 nodes }
906 \begin{tabular}{|*{7}{r|}}
908 Program & Execution & Energy & Energy & Performance & Distance \\
909 name & time/s & consumption/J & saving\% & degradation\% & \\
911 CG &56.92 &41163.36 &4.00 &1.10 &2.90 \\
913 MG &3.55 &2843.33 &18.77 &10.38 &8.39 \\
915 EP &2.67 &5669.66 &27.09 &0.03 &27.06 \\
917 LU &51.23 &144471.90 &16.67 &2.36 &14.31 \\
919 BT &37.96 &44243.82 &23.18 &1.28 &21.90 \\
921 SP &64.53 &115409.71 &26.72 &0.05 &26.67 \\
923 FT &25.51 &18808.72 &12.85 &2.84 &10.01 \\
926 \label{table:res_128n}
928 The overall energy consumption was computed for each instance according to the
929 energy consumption model (\ref{eq:energy}), with and without applying the
930 algorithm. The execution time was also measured for all these experiments. Then,
931 the energy saving and performance degradation percentages were computed for each
932 instance. The results are presented in Tables (\ref{table:res_4n},
933 \ref{table:res_8n}, \ref{table:res_16n}, \ref{table:res_32n},
934 \ref{table:res_64n} and \ref{table:res_128n}). All these results are the average
935 values from many experiments for energy savings and performance degradation.
936 The tables show the experimental results for running the NAS parallel benchmarks
937 on different number of nodes. The experiments show that the algorithm
938 significantly reduces the energy consumption (up to 35\%) and tries to limit the
939 performance degradation. They also show that the energy saving percentage
940 decreases when the number of computing nodes increases. This reduction is due
941 to the increase of the communication times compared to the execution times when
942 the benchmarks are run over a high number of nodes. Indeed, the benchmarks with
943 the same class, C, are executed on different numbers of nodes, so the
944 computation required for each iteration is divided by the number of computing
945 nodes. On the other hand, more communications are required when increasing the
946 number of nodes so the static energy increases linearly according to the
947 communication time and the dynamic power is less relevant in the overall energy
948 consumption. Therefore, reducing the frequency with algorithm~(\ref{HSA}) is
949 less effective in reducing the overall energy savings. It can also be noticed
950 that for the benchmarks EP and SP that contain little or no communications, the
951 energy savings are not significantly affected by the high number of nodes. No
952 experiments were conducted using bigger classes than D, because they require a
953 lot of memory (more than 64GB) when being executed by the simulator on one
954 machine. The maximum distance between the normalized energy curve and the
955 normalized performance for each instance is also shown in the result tables. It
956 decrease in the same way as the energy saving percentage. The tables also show
957 that the performance degradation percentage is not significantly increased when
958 the number of computing nodes is increased because the computation times are
959 small when compared to the communication times.
965 \subfloat[Energy saving]{%
966 \includegraphics[width=.33\textwidth]{fig/energy}\label{fig:energy}}%
968 \subfloat[Performance degradation ]{%
969 \includegraphics[width=.33\textwidth]{fig/per_deg}\label{fig:per_deg}}
971 \caption{The energy and performance for all NAS benchmarks running with a different number of nodes}
974 Figures \ref{fig:energy} and \ref{fig:per_deg} present the energy saving and
975 performance degradation respectively for all the benchmarks according to the
976 number of used nodes. As shown in the first plot, the energy saving percentages
977 of the benchmarks MG, LU, BT and FT decrease linearly when the number of nodes
978 increase. While for the EP and SP benchmarks, the energy saving percentage is
979 not affected by the increase of the number of computing nodes, because in these
980 benchmarks there are little or no communications. Finally, the energy saving of
981 the GC benchmark significantly decrease when the number of nodes increase
982 because this benchmark has more communications than the others. The second plot
983 shows that the performance degradation percentages of most of the benchmarks
984 decrease when they run on a big number of nodes because they spend more time
985 communicating than computing, thus, scaling down the frequencies of some nodes
986 has less effect on the performance.
991 \subsection{The results for different power consumption scenarios}
993 The results of the previous section were obtained while using processors that
994 consume during computation an overall power which is 80\% composed of dynamic
995 power and of 20\% of static power. In this section, these ratios are changed and
996 two new power scenarios are considered in order to evaluate how the proposed
997 algorithm adapts itself according to the static and dynamic power values. The
998 two new power scenarios are the following:
1001 \item 70\% of dynamic power and 30\% of static power
1002 \item 90\% of dynamic power and 10\% of static power
1005 The NAS parallel benchmarks were executed again over processors that follow the
1006 new power scenarios. The class C of each benchmark was run over 8 or 9 nodes
1007 and the results are presented in Tables \ref{table:res_s1} and
1008 \ref{table:res_s2}. These tables show that the energy saving percentage of the
1009 70\%-30\% scenario is smaller for all benchmarks compared to the energy saving
1010 of the 90\%-10\% scenario. Indeed, in the latter more dynamic power is consumed
1011 when nodes are running on their maximum frequencies, thus, scaling down the
1012 frequency of the nodes results in higher energy savings than in the 70\%-30\%
1013 scenario. On the other hand, the performance degradation percentage is smaller
1014 in the 70\%-30\% scenario compared to the 90\%-10\% scenario. This is due to the
1015 higher static power percentage in the first scenario which makes it more
1016 relevant in the overall consumed energy. Indeed, the static energy is related
1017 to the execution time and if the performance is degraded the amount of consumed
1018 static energy directly increases. Therefore, the proposed algorithm does not
1019 really significantly scale down much the frequencies of the nodes in order to
1020 limit the increase of the execution time and thus limiting the effect of the
1021 consumed static energy.
1023 Both new power scenarios are compared to the old one in figure
1024 (\ref{fig:sen_comp}). It shows the average of the performance degradation, the
1025 energy saving and the distances for all NAS benchmarks of class C running on 8
1026 or 9 nodes. The comparison shows that the energy saving ratio is proportional
1027 to the dynamic power ratio: it is increased when applying the 90\%-10\% scenario
1028 because at maximum frequency the dynamic energy is the most relevant in the
1029 overall consumed energy and can be reduced by lowering the frequency of some
1030 processors. On the other hand, the energy saving decreases when the 70\%-30\%
1031 scenario is used because the dynamic energy is less relevant in the overall
1032 consumed energy and lowering the frequency does not return big energy savings.
1033 Moreover, the average of the performance degradation is decreased when using a
1034 higher ratio for static power (e.g. 70\%-30\% scenario and 80\%-20\%
1035 scenario). Since the proposed algorithm optimizes the energy consumption when
1036 using a higher ratio for dynamic power the algorithm selects bigger frequency
1037 scaling factors that result in more energy saving but less performance, for
1038 example see Figure (\ref{fig:scales_comp}). The opposite happens when using a
1039 higher ratio for static power, the algorithm proportionally selects smaller
1040 scaling values which result in less energy saving but also less performance
1045 \caption{The results of the 70\%-30\% power scenario}
1048 \begin{tabular}{|*{6}{r|}}
1050 Program & Energy & Energy & Performance & Distance \\
1051 name & consumption/J & saving\% & degradation\% & \\
1053 CG &4144.21 &22.42 &7.72 &14.70 \\
1055 MG &1133.23 &24.50 &5.34 &19.16 \\
1057 EP &6170.30 &16.19 &0.02 &16.17 \\
1059 LU &39477.28 &20.43 &0.07 &20.36 \\
1061 BT &26169.55 &25.34 &6.62 &18.71 \\
1063 SP &19620.09 &19.32 &3.66 &15.66 \\
1065 FT &6094.07 &23.17 &0.36 &22.81 \\
1068 \label{table:res_s1}
1074 \caption{The results of the 90\%-10\% power scenario}
1077 \begin{tabular}{|*{6}{r|}}
1079 Program & Energy & Energy & Performance & Distance \\
1080 name & consumption/J & saving\% & degradation\% & \\
1082 CG &2812.38 &36.36 &6.80 &29.56 \\
1084 MG &825.427 &38.35 &6.41 &31.94 \\
1086 EP &5281.62 &35.02 &2.68 &32.34 \\
1088 LU &31611.28 &39.15 &3.51 &35.64 \\
1090 BT &21296.46 &36.70 &6.60 &30.10 \\
1092 SP &15183.42 &35.19 &11.76 &23.43 \\
1094 FT &3856.54 &40.80 &5.67 &35.13 \\
1097 \label{table:res_s2}
1103 \subfloat[Comparison between the results on 8 nodes]{%
1104 \includegraphics[width=.33\textwidth]{fig/sen_comp}\label{fig:sen_comp}}%
1106 \subfloat[Comparison the selected frequency scaling factors of MG benchmark class C running on 8 nodes]{%
1107 \includegraphics[width=.33\textwidth]{fig/three_scenarios}\label{fig:scales_comp}}
1109 \caption{The comparison of the three power scenarios}
1115 \subsection{The comparison of the proposed scaling algorithm }
1116 \label{sec.compare_EDP}
1117 In this section, the scaling factors selection algorithm, called MaxDist,
1118 is compared to Spiliopoulos et al. algorithm \cite{Spiliopoulos_Green.governors.Adaptive.DVFS}, called EDP.
1119 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.
1120 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
1121 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.
1123 Both algorithms were applied to the parallel NAS benchmarks to compare their efficiency. Table \ref{table:compare_EDP} presents the results of comparing the execution times and the energy consumption for both versions of the NAS benchmarks while running the class C of each benchmark over 8 or 9 heterogeneous nodes. The results show that our algorithm provides better energy savings than Spiliopoulos et al. algorithm,
1124 on average it results in 29.76\% energy saving while their algorithm returns just 25.75\%. The average of performance degradation percentage is approximately the same for both algorithms, about 4\%.
1127 For all benchmarks, our algorithm outperforms Spiliopoulos et al. algorithm in
1128 terms of energy and performance trade-off, see figure (\ref{fig:compare_EDP}),
1129 because it maximizes the distance between the energy saving and the performance
1130 degradation values while giving the same weight for both metrics.
1136 \caption{Comparing the proposed algorithm}
1138 \begin{tabular}{|*{7}{r|}}
1140 Program & \multicolumn{2}{c|}{Energy saving \%} & \multicolumn{2}{c|}{Perf. degradation \%} & \multicolumn{2}{c|}{Distance} \\ \cline{2-7}
1141 name & EDP & MaxDist & EDP & MaxDist & EDP & MaxDist \\ \hline
1142 CG & 27.58 & 31.25 & 5.82 & 7.12 & 21.76 & 24.13 \\ \hline
1143 MG & 29.49 & 33.78 & 3.74 & 6.41 & 25.75 & 27.37 \\ \hline
1144 LU & 19.55 & 28.33 & 0.0 & 0.01 & 19.55 & 28.22 \\ \hline
1145 EP & 28.40 & 27.04 & 4.29 & 0.49 & 24.11 & 26.55 \\ \hline
1146 BT & 27.68 & 32.32 & 6.45 & 7.87 & 21.23 & 24.43 \\ \hline
1147 SP & 20.52 & 24.73 & 5.21 & 2.78 & 15.31 & 21.95 \\ \hline
1148 FT & 27.03 & 31.02 & 2.75 & 2.54 & 24.28 & 28.48 \\ \hline
1151 \label{table:compare_EDP}
1160 \includegraphics[scale=0.5]{fig/compare_EDP.pdf}
1161 \caption{Trade-off comparison for NAS benchmarks class C}
1162 \label{fig:compare_EDP}
1166 \section{Conclusion}
1168 In this paper, a new online frequency selecting algorithm has been presented. It
1169 selects the best possible vector of frequency scaling factors that gives the
1170 maximum distance (optimal trade-off) between the predicted energy and the
1171 predicted performance curves for a heterogeneous platform. This algorithm uses a
1172 new energy model for measuring and predicting the energy of distributed
1173 iterative applications running over heterogeneous platforms. To evaluate the
1174 proposed method, it was applied on the NAS parallel benchmarks and executed over
1175 a heterogeneous platform simulated by SimGrid. The results of the experiments
1176 showed that the algorithm reduces up to 35\% the energy consumption of a message
1177 passing iterative method while limiting the degradation of the performance. The
1178 algorithm also selects different scaling factors according to the percentage of
1179 the computing and communication times, and according to the values of the static
1180 and dynamic powers of the CPUs. Finally, the algorithm was compared to
1181 Spiliopoulos et al. algorithm and the results showed that it outperforms their
1182 algorithm in terms of energy-time trade-off.
1184 In the near future, this method will be applied to real heterogeneous platforms
1185 to evaluate its performance in a real study case. It would also be interesting
1186 to evaluate its scalability over large scale heterogeneous platforms and measure
1187 the energy consumption reduction it can produce. Afterward, we would like to
1188 develop a similar method that is adapted to asynchronous iterative applications
1189 where each task does not wait for other tasks to finish their works. The
1190 development of such a method might require a new energy model because the number
1191 of iterations is not known in advance and depends on the global convergence of
1192 the iterative system.
1194 \section*{Acknowledgment}
1196 This work has been partially supported by the Labex
1197 ACTION project (contract “ANR-11-LABX-01-01”). As a PhD student,
1198 Mr. Ahmed Fanfakh, would like to thank the University of
1199 Babylon (Iraq) for supporting his work.
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1219 % LocalWords: Fanfakh Charr FIXME Tianhe DVFS HPC NAS NPB SMPI Rauber's Rauber
1220 % LocalWords: CMOS EPSA Franche Comté Tflop Rünger IUT Maréchal Juin cedex GPU
1221 % LocalWords: de badri muslim MPI TcpOld TcmOld dNew dOld cp Sopt Tcp Tcm Ps
1222 % LocalWords: Scp Fmax Fdiff SimGrid GFlops Xeon EP BT GPUs CPUs AMD
1223 % LocalWords: Spiliopoulos scalability