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56 \title{Energy Consumption Reduction for Message Passing Iterative Applications in Heterogeneous Architecture Using DVFS}
66 FEMTO-ST Institute, University of Franche-Comte\\
67 IUT de Belfort-Montbéliard,
68 19 avenue du Maréchal Juin, BP 527, 90016 Belfort cedex, France\\
69 % Telephone: \mbox{+33 3 84 58 77 86}, % Raphaël
70 % Fax: \mbox{+33 3 84 58 77 81}\\ % Dept Info
71 Email: \email{{jean-claude.charr,raphael.couturier,ahmed.fanfakh_badri_muslim,arnaud.giersch}@univ-fcomte.fr}
78 Computing platforms are consuming more and more energy due to the increasing
79 number of nodes composing them. To minimize the operating costs of these
80 platforms many techniques have been used. Dynamic voltage and frequency scaling
81 (DVFS) is one of them. It reduces the frequency of a CPU to lower its energy
82 consumption. However, lowering the frequency of a CPU might increase the
83 execution time of an application running on that processor. Therefore, the
84 frequency that gives the best tradeoff between the energy consumption and the
85 performance of an application must be selected.\\
86 In this paper, a new online frequencies selecting algorithm for heterogeneous
87 platforms is presented. It selects the frequency which tries to give the best
88 tradeoff between energy saving and performance degradation, for each node
89 computing the message passing iterative application. The algorithm has a small
90 overhead and works without training or profiling. It uses a new energy model for
91 message passing iterative applications running on a heterogeneous platform. The
92 proposed algorithm is evaluated on the Simgrid simulator while running the NAS
93 parallel benchmarks. The experiments show that it reduces the energy
94 consumption by up to 35\% while limiting the performance degradation as much as
95 possible. Finally, the algorithm is compared to an existing method, the
96 comparison results showing that it outperforms the latter.
100 \section{Introduction}
102 The need for more computing power is continually increasing. To partially
103 satisfy this need, most supercomputers constructors just put more computing
104 nodes in their platform. The resulting platforms might achieve higher floating
105 point operations per second (FLOPS), but the energy consumption and the heat
106 dissipation are also increased. As an example, the Chinese supercomputer
107 Tianhe-2 had the highest FLOPS in November 2014 according to the Top500 list
108 \cite{TOP500_Supercomputers_Sites}. However, it was also the most power hungry
109 platform with its over 3 million cores consuming around 17.8 megawatts.
110 Moreover, according to the U.S. annual energy outlook 2014
111 \cite{U.S_Annual.Energy.Outlook.2014}, the price of energy for 1 megawatt-hour
112 was approximately equal to \$70. Therefore, the price of the energy consumed by
113 the Tianhe-2 platform is approximately more than \$10 million each year. The
114 computing platforms must be more energy efficient and offer the highest number
115 of FLOPS per watt possible, such as the L-CSC from the GSI Helmholtz Center
116 which became the top of the Green500 list in November 2014 \cite{Green500_List}.
117 This heterogeneous platform executes more than 5 GFLOPS per watt while consuming
120 Besides platform improvements, there are many software and hardware techniques
121 to lower the energy consumption of these platforms, such as scheduling, DVFS,
122 ... DVFS is a widely used process to reduce the energy consumption of a
123 processor by lowering its frequency
124 \cite{Rizvandi_Some.Observations.on.Optimal.Frequency}. However, it also reduces
125 the number of FLOPS executed by the processor which might increase the execution
126 time of the application running over that processor. Therefore, researchers use
127 different optimization strategies to select the frequency that gives the best
128 tradeoff between the energy reduction and performance degradation ratio. In
129 \cite{Our_first_paper}, a frequency selecting algorithm was proposed to reduce
130 the energy consumption of message passing iterative applications running over
131 homogeneous platforms. The results of the experiments show significant energy
132 consumption reductions. In this paper, a new frequency selecting algorithm
133 adapted for heterogeneous platform is presented. It selects the vector of
134 frequencies, for a heterogeneous platform running a message passing iterative
135 application, that simultaneously tries to offer the maximum energy reduction and
136 minimum performance degradation ratio. The algorithm has a very small overhead,
137 works online and does not need any training or profiling.
139 This paper is organized as follows: Section~\ref{sec.relwork} presents some
140 related works from other authors. Section~\ref{sec.exe} describes how the
141 execution time of message passing programs can be predicted. It also presents an energy
142 model that predicts the energy consumption of an application running over a heterogeneous platform. Section~\ref{sec.compet} presents
143 the energy-performance objective function that maximizes the reduction of energy
144 consumption while minimizing the degradation of the program's performance.
145 Section~\ref{sec.optim} details the proposed frequency selecting algorithm then the precision of the proposed algorithm is verified.
146 Section~\ref{sec.expe} presents the results of applying the algorithm on the NAS parallel benchmarks and executing them
147 on a heterogeneous platform. It shows the results of running three
148 different power scenarios and comparing them. Moreover, it also shows the comparison results
149 between the proposed method and an existing method.
150 Finally, in Section~\ref{sec.concl} the paper ends with a summary and some future works.
152 \section{Related works}
154 DVFS is a technique used in modern processors to scale down both the voltage and
155 the frequency of the CPU while computing, in order to reduce the energy
156 consumption of the processor. DVFS is also allowed in GPUs to achieve the
157 same goal. Reducing the frequency of a processor lowers its number of FLOPS and
158 might degrade the performance of the application running on that processor,
159 especially if it is compute bound. Therefore selecting the appropriate frequency
160 for a processor to satisfy some objectives while taking into account all the
161 constraints, is not a trivial operation. Many researchers used different
162 strategies to tackle this problem. Some of them developed online methods that
163 compute the new frequency while executing the application, such as
164 ~\cite{Hao_Learning.based.DVFS,Spiliopoulos_Green.governors.Adaptive.DVFS}. Others
165 used offline methods that might need to run the application and profile it
166 before selecting the new frequency, such as
167 ~\cite{Rountree_Bounding.energy.consumption.in.MPI,Cochran_Pack_and_Cap_Adaptive_DVFS}. The
168 methods could be heuristics, exact or brute force methods that satisfy varied
169 objectives such as energy reduction or performance. They also could be adapted
170 to the execution's environment and the type of the application such as
171 sequential, parallel or distributed architecture, homogeneous or heterogeneous
172 platform, synchronous or asynchronous application, ...
174 In this paper, we are interested in reducing energy for message passing iterative synchronous applications running over heterogeneous platforms.
175 Some works have already been done for such platforms and they can be classified into two types of heterogeneous platforms:
178 \item the platform is composed of homogeneous GPUs and homogeneous CPUs.
179 \item the platform is only composed of heterogeneous CPUs.
183 For the first type of platform, the computing intensive parallel tasks are executed on the GPUs and the rest are executed
184 on the CPUs. Luley et al.
185 ~\cite{Luley_Energy.efficiency.evaluation.and.benchmarking}, proposed a heterogeneous
186 cluster composed of Intel Xeon CPUs and NVIDIA GPUs. Their main goal was to maximize the
187 energy efficiency of the platform during computation by maximizing the number of FLOPS per watt generated.
188 In~\cite{KaiMa_Holistic.Approach.to.Energy.Efficiency.in.GPU-CPU}, Kai Ma et al. developed a scheduling
189 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.
190 In~\cite{Rong_Effects.of.DVFS.on.K20.GPU}, Rong et al. showed that
191 a heterogeneous (GPUs and CPUs) cluster that enables DVFS gave better energy and performance
192 efficiency than other clusters only composed of CPUs.
194 The work presented in this paper concerns the second type of platform, with heterogeneous CPUs.
195 Many methods were conceived to reduce the energy consumption of this type of platform. Naveen et al.~\cite{Naveen_Power.Efficient.Resource.Scaling}
196 developed a method that minimizes the value of $energy*delay^2$ (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
197 an algorithm that divides the executed tasks into two types: the critical and
198 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
199 a heterogeneous cluster composed of two types
200 of Intel and AMD processors. They use a gradient method to predict the impact of DVFS operations on performance.
201 In~\cite{Shelepov_Scheduling.on.Heterogeneous.Multicore} and \cite{Li_Minimizing.Energy.Consumption.for.Frame.Based.Tasks},
202 the best frequencies for a specified heterogeneous cluster are selected offline using some
203 heuristic. Chen et al.~\cite{Chen_DVFS.under.quality.of.service.requirements} used a greedy dynamic programming approach to
204 minimize the power consumption of heterogeneous servers while respecting given time constraints. This approach
205 had considerable overhead.
206 In contrast to the above described papers, this paper presents the following contributions :
208 \item two new energy and performance models for message passing iterative synchronous applications running over
209 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.
211 \item a new online frequency selecting algorithm for heterogeneous platforms. The algorithm has a very small
212 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.
216 \section{The performance and energy consumption measurements on heterogeneous architecture}
221 \subsection{The execution time of message passing distributed
222 iterative applications on a heterogeneous platform}
224 In this paper, we are interested in reducing the energy consumption of message
225 passing distributed iterative synchronous applications running over
226 heterogeneous platforms. A heterogeneous platform is defined as a collection of
227 heterogeneous computing nodes interconnected via a high speed homogeneous
228 network. Therefore, each node has different characteristics such as computing
229 power (FLOPS), energy consumption, CPU's frequency range, \dots{} but they all
230 have the same network bandwidth and latency.
232 The overall execution time of a distributed iterative synchronous application
233 over a heterogeneous platform consists of the sum of the computation time and
234 the communication time for every iteration on a node. However, due to the
235 heterogeneous computation power of the computing nodes, slack times might occur
236 when fast nodes have to wait, during synchronous communications, for the slower
237 nodes to finish their computations (see Figure~(\ref{fig:heter})).
238 Therefore, the overall execution time of the program is the execution time of the slowest
239 task which has the highest computation time and no slack time.
243 \includegraphics[scale=0.6]{fig/commtasks}
244 \caption{Parallel tasks on a heterogeneous platform}
248 Dynamic Voltage and Frequency Scaling (DVFS) is a process, implemented in
249 modern processors, that reduces the energy consumption of a CPU by scaling
250 down its voltage and frequency. Since DVFS lowers the frequency of a CPU
251 and consequently its computing power, the execution time of a program running
252 over that scaled down processor might increase, especially if the program is
253 compute bound. The frequency reduction process can be expressed by the scaling
254 factor S which is the ratio between the maximum and the new frequency of a CPU
258 S = \frac{F_\textit{max}}{F_\textit{new}}
260 The execution time of a compute bound sequential program is linearly proportional
261 to the frequency scaling factor $S$. On the other hand, message passing
262 distributed applications consist of two parts: computation and communication.
263 The execution time of the computation part is linearly proportional to the
264 frequency scaling factor $S$ but the communication time is not affected by the
265 scaling factor because the processors involved remain idle during the
266 communications~\cite{Freeh_Exploring.the.Energy.Time.Tradeoff}.
267 The communication time for a task is the summation of periods of
268 time that begin with an MPI call for sending or receiving a message
269 until the message is synchronously sent or received.
271 Since in a heterogeneous platform each node has different characteristics,
272 especially different frequency gears, when applying DVFS operations on these
273 nodes, they may get different scaling factors represented by a scaling vector:
274 $(S_1, S_2,\dots, S_N)$ where $S_i$ is the scaling factor of processor $i$. To
275 be able to predict the execution time of message passing synchronous iterative
276 applications running over a heterogeneous platform, for different vectors of
277 scaling factors, the communication time and the computation time for all the
278 tasks must be measured during the first iteration before applying any DVFS
279 operation. Then the execution time for one iteration of the application with any
280 vector of scaling factors can be predicted using (\ref{eq:perf}).
283 \textit T_\textit{new} =
284 \max_{i=1,2,\dots,N} ({TcpOld_{i}} \cdot S_{i}) + MinTcm
289 MinTcm = \min_{i=1,2,\dots,N} (Tcm_i)
291 where $TcpOld_i$ is the computation time of processor $i$ during the first
292 iteration and $MinTcm$ is the communication time of the slowest processor from
293 the first iteration. The model computes the maximum computation time with
294 scaling factor from each node added to the communication time of the slowest
295 node. It means only the communication time without any slack time is taken into
296 account. Therefore, the execution time of the iterative application is equal to
297 the execution time of one iteration as in (\ref{eq:perf}) multiplied by the
298 number of iterations of that application.
300 This prediction model is developed from the model to predict the execution time
301 of message passing distributed applications for homogeneous
302 architectures~\cite{Our_first_paper}. The execution time prediction model is
303 used in the method to optimize both the energy consumption and the performance of
304 iterative methods, which is presented in the following sections.
307 \subsection{Energy model for heterogeneous platform}
308 Many researchers~\cite{Malkowski_energy.efficient.high.performance.computing,
309 Rauber_Analytical.Modeling.for.Energy,Zhuo_Energy.efficient.Dynamic.Task.Scheduling,
310 Rizvandi_Some.Observations.on.Optimal.Frequency} divide the power consumed by a processor into
311 two power metrics: the static and the dynamic power. While the first one is
312 consumed as long as the computing unit is turned on, the latter is only consumed during
313 computation times. The dynamic power $Pd$ is related to the switching
314 activity $\alpha$, load capacitance $C_L$, the supply voltage $V$ and
315 operational frequency $F$, as shown in (\ref{eq:pd}).
318 Pd = \alpha \cdot C_L \cdot V^2 \cdot F
320 The static power $Ps$ captures the leakage power as follows:
323 Ps = V \cdot N_{trans} \cdot K_{design} \cdot I_{leak}
325 where V is the supply voltage, $N_{trans}$ is the number of transistors,
326 $K_{design}$ is a design dependent parameter and $I_{leak}$ is a
327 technology dependent parameter. The energy consumed by an individual processor
328 to execute a given program can be computed as:
331 E_\textit{ind} = Pd \cdot Tcp + Ps \cdot T
333 where $T$ is the execution time of the program, $Tcp$ is the computation
334 time and $Tcp \le T$. $Tcp$ may be equal to $T$ if there is no
335 communication and no slack time.
337 The main objective of DVFS operation is to reduce the overall energy consumption~\cite{Le_DVFS.Laws.of.Diminishing.Returns}.
338 The operational frequency $F$ depends linearly on the supply voltage $V$, i.e., $V = \beta \cdot F$ with some
339 constant $\beta$.~This equation is used to study the change of the dynamic
340 voltage with respect to various frequency values in~\cite{Rauber_Analytical.Modeling.for.Energy}. The reduction
341 process of the frequency can be expressed by the scaling factor $S$ which is the
342 ratio between the maximum and the new frequency as in (\ref{eq:s}).
343 The CPU governors are power schemes supplied by the operating
344 system's kernel to lower a core's frequency. The new frequency
345 $F_{new}$ from (\ref{eq:s}) can be calculated as follows:
348 F_\textit{new} = S^{-1} \cdot F_\textit{max}
350 Replacing $F_{new}$ in (\ref{eq:pd}) as in (\ref{eq:fnew}) gives the following
351 equation for dynamic power consumption:
354 {P}_\textit{dNew} = \alpha \cdot C_L \cdot V^2 \cdot F_{new} = \alpha \cdot C_L \cdot \beta^2 \cdot F_{new}^3 \\
355 {} = \alpha \cdot C_L \cdot V^2 \cdot F_{max} \cdot S^{-3} = P_{dOld} \cdot S^{-3}
357 where $ {P}_\textit{dNew}$ and $P_{dOld}$ are the dynamic power consumed with the
358 new frequency and the maximum frequency respectively.
360 According to (\ref{eq:pdnew}) the dynamic power is reduced by a factor of $S^{-3}$ when
361 reducing the frequency by a factor of $S$~\cite{Rauber_Analytical.Modeling.for.Energy}. Since the FLOPS of a CPU is proportional
362 to the frequency of a CPU, the computation time is increased proportionally to $S$.
363 The new dynamic energy is the dynamic power multiplied by the new time of computation
364 and is given by the following equation:
367 E_\textit{dNew} = P_{dOld} \cdot S^{-3} \cdot (Tcp \cdot S)= S^{-2}\cdot P_{dOld} \cdot Tcp
369 The static power is related to the power leakage of the CPU and is consumed during computation
370 and even when idle. As in~\cite{Rauber_Analytical.Modeling.for.Energy,Zhuo_Energy.efficient.Dynamic.Task.Scheduling},
371 the static power of a processor is considered as constant
372 during idle and computation periods, and for all its available frequencies.
373 The static energy is the static power multiplied by the execution time of the program.
374 According to the execution time model in (\ref{eq:perf}), the execution time of the program
375 is the sum of the computation and the communication times. The computation time is linearly related
376 to the frequency scaling factor, while this scaling factor does not affect the communication time.
377 The static energy of a processor after scaling its frequency is computed as follows:
380 E_\textit{s} = Ps \cdot (Tcp \cdot S + Tcm)
383 In the considered heterogeneous platform, each processor $i$ might have
384 different dynamic and static powers, noted as $Pd_{i}$ and $Ps_{i}$
385 respectively. Therefore, even if the distributed message passing iterative
386 application is load balanced, the computation time of each CPU $i$ noted
387 $Tcp_{i}$ might be different and different frequency scaling factors might be
388 computed in order to decrease the overall energy consumption of the application
389 and reduce slack times. The communication time of a processor $i$ is noted as
390 $Tcm_{i}$ and could contain slack times when communicating with slower
391 nodes, see figure(\ref{fig:heter}). Therefore, all nodes do not have equal
392 communication times. While the dynamic energy is computed according to the
393 frequency scaling factor and the dynamic power of each node as in
394 (\ref{eq:Edyn}), the static energy is computed as the sum of the execution time
395 of one iteration multiplied by the static power of each processor. The overall
396 energy consumption of a message passing distributed application executed over a
397 heterogeneous platform during one iteration is the summation of all dynamic and
398 static energies for each processor. It is computed as follows:
401 E = \sum_{i=1}^{N} {(S_i^{-2} \cdot Pd_{i} \cdot Tcp_i)} + {} \\
402 \sum_{i=1}^{N} (Ps_{i} \cdot (\max_{i=1,2,\dots,N} (Tcp_i \cdot S_{i}) +
406 Reducing the frequencies of the processors according to the vector of
407 scaling factors $(S_1, S_2,\dots, S_N)$ may degrade the performance of the
408 application and thus, increase the static energy because the execution time is
409 increased~\cite{Kim_Leakage.Current.Moore.Law}. The overall energy consumption for the iterative
410 application can be measured by measuring the energy consumption for one iteration as in (\ref{eq:energy})
411 multiplied by the number of iterations of that application.
414 \section{Optimization of both energy consumption and performance}
417 Using the lowest frequency for each processor does not necessarily give the most
418 energy efficient execution of an application. Indeed, even though the dynamic
419 power is reduced while scaling down the frequency of a processor, its
420 computation power is proportionally decreased. Hence, the execution time might
421 be drastically increased and during that time, dynamic and static powers are
422 being consumed. Therefore, it might cancel any gains achieved by scaling down
423 the frequency of all nodes to the minimum and the overall energy consumption of
424 the application might not be the optimal one. It is not trivial to select the
425 appropriate frequency scaling factor for each processor while considering the
426 characteristics of each processor (computation power, range of frequencies,
427 dynamic and static powers) and the task executed (computation/communication
428 ratio). The aim being to reduce the overall energy consumption and to avoid
429 increasing significantly the execution time. In our previous
430 work~\cite{Our_first_paper}, we proposed a method that selects the optimal
431 frequency scaling factor for a homogeneous cluster executing a message passing
432 iterative synchronous application while giving the best trade-off between the
433 energy consumption and the performance for such applications. In this work we
434 are interested in heterogeneous clusters as described above. Due to the
435 heterogeneity of the processors, a vector of scaling factors should
436 be selected and it must give the best trade-off between energy consumption and
439 The relation between the energy consumption and the execution time for an
440 application is complex and nonlinear, Thus, unlike the relation between the
441 execution time and the scaling factor, the relation between the energy and the
442 frequency scaling factors is nonlinear, for more details refer
443 to~\cite{Freeh_Exploring.the.Energy.Time.Tradeoff}. Moreover, these relations
444 are not measured using the same metric. To solve this problem, the execution
445 time is normalized by computing the ratio between the new execution time (after
446 scaling down the frequencies of some processors) and the initial one (with
447 maximum frequency for all nodes) as follows:
450 P_\textit{Norm} = \frac{T_\textit{New}}{T_\textit{Old}}\\
451 {} = \frac{ \max_{i=1,2,\dots,N} (Tcp_{i} \cdot S_{i}) +MinTcm}
452 {\max_{i=1,2,\dots,N}{(Tcp_i+Tcm_i)}}
456 In the same way, the energy is normalized by computing the ratio between the consumed energy
457 while scaling down the frequency and the consumed energy with maximum frequency for all nodes:
460 E_\textit{Norm} = \frac{E_\textit{Reduced}}{E_\textit{Original}} \\
461 {} = \frac{ \sum_{i=1}^{N}{(S_i^{-2} \cdot Pd_i \cdot Tcp_i)} +
462 \sum_{i=1}^{N} {(Ps_i \cdot T_{New})}}{\sum_{i=1}^{N}{( Pd_i \cdot Tcp_i)} +
463 \sum_{i=1}^{N} {(Ps_i \cdot T_{Old})}}
465 Where $E_\textit{Reduced}$ and $E_\textit{Original}$ are computed using (\ref{eq:energy}) and
466 $T_{New}$ and $T_{Old}$ are computed as in (\ref{eq:pnorm}).
469 goal is to optimize the energy and execution time at the same time, the normalized
470 energy and execution time curves are not in the same direction. According
471 to the equations~(\ref{eq:pnorm}) and (\ref{eq:enorm}), the vector of frequency
472 scaling factors $S_1,S_2,\dots,S_N$ reduce both the energy and the execution
473 time simultaneously. But the main objective is to produce maximum energy
474 reduction with minimum execution time reduction.
476 This problem can be solved by making the optimization process for energy and
477 execution time following the same direction. Therefore, the equation of the
478 normalized execution time is inverted which gives the normalized performance equation, as follows:
481 P_\textit{Norm} = \frac{T_\textit{Old}}{T_\textit{New}}\\
482 = \frac{\max_{i=1,2,\dots,N}{(Tcp_i+Tcm_i)}}
483 { \max_{i=1,2,\dots,N} (Tcp_{i} \cdot S_{i}) + MinTcm}
489 \subfloat[Homogeneous platform]{%
490 \includegraphics[width=.33\textwidth]{fig/homo}\label{fig:r1}}%
493 \subfloat[Heterogeneous platform]{%
494 \includegraphics[width=.33\textwidth]{fig/heter}\label{fig:r2}}
496 \caption{The energy and performance relation}
499 Then, the objective function can be modeled in order to find the maximum distance
500 between the energy curve (\ref{eq:enorm}) and the performance
501 curve (\ref{eq:pnorm_inv}) over all available sets of scaling factors. This
502 represents the minimum energy consumption with minimum execution time (maximum
503 performance) at the same time, see figure~(\ref{fig:r1}) or figure~(\ref{fig:r2}). Then the objective
504 function has the following form:
508 \max_{i=1,\dots F, j=1,\dots,N}
509 (\overbrace{P_\textit{Norm}(S_{ij})}^{\text{Maximize}} -
510 \overbrace{E_\textit{Norm}(S_{ij})}^{\text{Minimize}} )
512 where $N$ is the number of nodes and $F$ is the number of available frequencies for each node.
513 Then, the optimal set of scaling factors that satisfies (\ref{eq:max}) can be selected.
514 The objective function can work with any energy model or any power values for each node
515 (static and dynamic powers). However, the most important energy reduction gain can be achieved when
516 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}.
518 \section{The scaling factors selection algorithm for heterogeneous platforms }
521 \subsection{The algorithm details}
522 In this section, algorithm \ref{HSA} is presented. It selects the frequency scaling factors
523 vector that gives the best trade-off between minimizing the energy consumption and maximizing
524 the performance of a message passing synchronous iterative application executed on a heterogeneous
525 platform. It works online during the execution time of the iterative message passing program.
526 It uses information gathered during the first iteration such as the computation time and the
527 communication time in one iteration for each node. The algorithm is executed after the first
528 iteration and returns a vector of optimal frequency scaling factors that satisfies the objective
529 function (\ref{eq:max}). The program applies DVFS operations to change the frequencies of the CPUs
530 according to the computed scaling factors. This algorithm is called just once during the execution
531 of the program. Algorithm~(\ref{dvfs}) shows where and when the proposed scaling algorithm is called
532 in the iterative MPI program.
534 The nodes in a heterogeneous platform have different computing powers, thus while executing message
535 passing iterative synchronous applications, fast nodes have to wait for the slower ones to finish their
536 computations before being able to synchronously communicate with them as in figure (\ref{fig:heter}).
537 These periods are called idle or slack times.
538 The algorithm takes into account this problem and tries to reduce these slack times when selecting the
539 frequency scaling factors vector. At first, it selects initial frequency scaling factors that increase
540 the execution times of fast nodes and minimize the differences between the computation times of
541 fast and slow nodes. The value of the initial frequency scaling factor for each node is inversely
542 proportional to its computation time that was gathered from the first iteration. These initial frequency
543 scaling factors are computed as a ratio between the computation time of the slowest node and the
544 computation time of the node $i$ as follows:
547 Scp_{i} = \frac{\max_{i=1,2,\dots,N}(Tcp_i)}{Tcp_i}
549 Using the initial frequency scaling factors computed in (\ref{eq:Scp}), the algorithm computes
550 the initial frequencies for all nodes as a ratio between the maximum frequency of node $i$
551 and the computation scaling factor $Scp_i$ as follows:
554 F_{i} = \frac{Fmax_i}{Scp_i},~{i=1,2,\cdots,N}
556 If the computed initial frequency for a node is not available in the gears of
557 that node, it is replaced by the nearest available frequency. In figure
558 (\ref{fig:st_freq}), the nodes are sorted by their computing power in ascending
559 order and the frequencies of the faster nodes are scaled down according to the
560 computed initial frequency scaling factors. The resulting new frequencies are
561 colored in blue in figure (\ref{fig:st_freq}). This set of frequencies can be
562 considered as a higher bound for the search space of the optimal vector of
563 frequencies because selecting frequency scaling factors higher than the higher
564 bound will not improve the performance of the application and it will increase
565 its overall energy consumption. Therefore the algorithm that selects the
566 frequency scaling factors starts the search method from these initial
567 frequencies and takes a downward search direction toward lower frequencies. The
568 algorithm iterates on all left frequencies, from the higher bound until all
569 nodes reach their minimum frequencies, to compute their overall energy
570 consumption and performance, and select the optimal frequency scaling factors
571 vector. At each iteration the algorithm determines the slowest node according to
572 the equation (\ref{eq:perf}) and keeps its frequency unchanged, while it lowers
573 the frequency of all other nodes by one gear. The new overall energy
574 consumption and execution time are computed according to the new scaling
575 factors. The optimal set of frequency scaling factors is the set that gives the
576 highest distance according to the objective function (\ref{eq:max}).
578 Figures~\ref{fig:r1} and \ref{fig:r2} illustrate the normalized performance and
579 consumed energy for an application running on a homogeneous platform and a
580 heterogeneous platform respectively while increasing the scaling factors. It can
581 be noticed that in a homogeneous platform the search for the optimal scaling
582 factor should start from the maximum frequency because the performance and the
583 consumed energy decrease from the beginning of the plot. On the other hand,
584 in the heterogeneous platform the performance is maintained at the beginning of
585 the plot even if the frequencies of the faster nodes decrease until the
586 computing power of scaled down nodes are lower than the slowest node. In other
587 words, until they reach the higher bound. It can also be noticed that the higher
588 the difference between the faster nodes and the slower nodes is, the bigger the
589 maximum distance between the energy curve and the performance curve is while
590 the scaling factors are varying which results in bigger energy savings.
593 \includegraphics[scale=0.5]{fig/start_freq}
594 \caption{Selecting the initial frequencies}
602 \begin{algorithmic}[1]
606 \item[$Tcp_i$] array of all computation times for all nodes during one iteration and with highest frequency.
607 \item[$Tcm_i$] array of all communication times for all nodes during one iteration and with highest frequency.
608 \item[$Fmax_i$] array of the maximum frequencies for all nodes.
609 \item[$Pd_i$] array of the dynamic powers for all nodes.
610 \item[$Ps_i$] array of the static powers for all nodes.
611 \item[$Fdiff_i$] array of the difference between two successive frequencies for all nodes.
613 \Ensure $Sopt_1,Sopt_2 \dots, Sopt_N$ is a vector of optimal scaling factors
615 \State $ Scp_i \gets \frac{\max_{i=1,2,\dots,N}(Tcp_i)}{Tcp_i} $
616 \State $F_{i} \gets \frac{Fmax_i}{Scp_i},~{i=1,2,\cdots,N}$
617 \State Round the computed initial frequencies $F_i$ to the closest one available in each node.
618 \If{(not the first frequency)}
619 \State $F_i \gets F_i+Fdiff_i,~i=1,\dots,N.$
621 \State $T_\textit{Old} \gets max_{~i=1,\dots,N } (Tcp_i+Tcm_i)$
622 \State $E_\textit{Original} \gets \sum_{i=1}^{N}{( Pd_i \cdot Tcp_i)} +\sum_{i=1}^{N} {(Ps_i \cdot T_{Old})}$
623 \State $Sopt_{i} \gets 1,~i=1,\dots,N. $
624 \State $Dist \gets 0 $
625 \While {(all nodes not reach their minimum frequency)}
626 \If{(not the last freq. \textbf{and} not the slowest node)}
627 \State $F_i \gets F_i - Fdiff_i,~i=1,\dots,N.$
628 \State $S_i \gets \frac{Fmax_i}{F_i},~i=1,\dots,N.$
630 \State $T_{New} \gets max_\textit{~i=1,\dots,N} (Tcp_{i} \cdot S_{i}) + MinTcm $
631 \State $E_\textit{Reduced} \gets \sum_{i=1}^{N}{(S_i^{-2} \cdot Pd_i \cdot Tcp_i)} + $ \hspace*{43 mm}
632 $\sum_{i=1}^{N} {(Ps_i \cdot T_{New})} $
633 \State $ P_\textit{Norm} \gets \frac{T_\textit{Old}}{T_\textit{New}}$
634 \State $E_\textit{Norm}\gets \frac{E_\textit{Reduced}}{E_\textit{Original}}$
635 \If{$(\Pnorm - \Enorm > \Dist)$}
636 \State $Sopt_{i} \gets S_{i},~i=1,\dots,N. $
637 \State $\Dist \gets \Pnorm - \Enorm$
640 \State Return $Sopt_1,Sopt_2,\dots,Sopt_N$
642 \caption{frequency scaling factors selection algorithm}
647 \begin{algorithmic}[1]
649 \For {$k=1$ to \textit{some iterations}}
650 \State Computations section.
651 \State Communications section.
653 \State Gather all times of computation and\newline\hspace*{3em}%
654 communication from each node.
655 \State Call algorithm \ref{HSA}.
656 \State Compute the new frequencies from the\newline\hspace*{3em}%
657 returned optimal scaling factors.
658 \State Set the new frequencies to nodes.
662 \caption{DVFS algorithm}
666 \subsection{The evaluation of the proposed algorithm}
667 \label{sec.verif.algo}
668 The precision of the proposed algorithm mainly depends on the execution time
669 prediction model defined in (\ref{eq:perf}) and the energy model computed by
670 (\ref{eq:energy}). The energy model is also significantly dependent on the
671 execution time model because the static energy is linearly related to the
672 execution time and the dynamic energy is related to the computation time. So,
673 all the works presented in this paper are based on the execution time model. To
674 verify this model, the predicted execution time was compared to the real
675 execution time over SimGrid/SMPI simulator,
676 v3.10~\cite{casanova+giersch+legrand+al.2014.versatile}, for all the NAS
677 parallel benchmarks NPB v3.3 \cite{NAS.Parallel.Benchmarks}, running class B on
678 8 or 9 nodes. The comparison showed that the proposed execution time model is
679 very precise, the maximum normalized difference between the predicted execution
680 time and the real execution time is equal to 0.03 for all the NAS benchmarks.
682 Since the proposed algorithm is not an exact method it does not test all the possible solutions (vectors of scaling factors)
683 in the search space. To prove its efficiency, it was compared on small instances to a brute force search algorithm
684 that tests all the possible solutions. The brute force algorithm was applied to different NAS benchmarks classes with
685 different number of nodes. The solutions returned by the brute force algorithm and the proposed algorithm were identical
686 and the proposed algorithm was on average 10 times faster than the brute force algorithm. It has a small execution time:
687 for a heterogeneous cluster composed of four different types of nodes having the characteristics presented in
688 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
689 to compute the best scaling factors vector. The algorithm complexity is $O(F\cdot (N \cdot4) )$, where $F$ is the number
690 of iterations and $N$ is the number of computing nodes. The algorithm needs from 12 to 20 iterations to select the best
691 vector of frequency scaling factors that gives the results of the next sections.
693 \section{Experimental results}
695 To evaluate the efficiency and the overall energy consumption reduction of
696 algorithm~\ref{HSA}, it was applied to the NAS parallel benchmarks NPB v3.3. The
697 experiments were executed on the simulator SimGrid/SMPI which offers easy tools
698 to create a heterogeneous platform and run message passing applications over it.
699 The heterogeneous platform that was used in the experiments, had one core per
700 node because just one process was executed per node. The heterogeneous platform
701 was composed of four types of nodes. Each type of nodes had different
702 characteristics such as the maximum CPU frequency, the number of available
703 frequencies and the computational power, see Table \ref{table:platform}. The
704 characteristics of these different types of nodes are inspired from the
705 specifications of real Intel processors. The heterogeneous platform had up to
706 144 nodes and had nodes from the four types in equal proportions, for example if
707 a benchmark was executed on 8 nodes, 2 nodes from each type were used. Since the
708 constructors of CPUs do not specify the dynamic and the static power of their
709 CPUs, for each type of node they were chosen proportionally to its computing
710 power (FLOPS). In the initial heterogeneous platform, while computing with
711 highest frequency, each node consumed an amount of power proportional to its
712 computing power (which corresponds to 80\% of its dynamic power and the
713 remaining 20\% to the static power), the same assumption was made in
714 \cite{Our_first_paper,Rauber_Analytical.Modeling.for.Energy}. Finally, These
715 nodes were connected via an ethernet network with 1 Gbit/s bandwidth.
719 \caption{Heterogeneous nodes characteristics}
722 \begin{tabular}{|*{7}{l|}}
724 Node &Simulated & Max & Min & Diff. & Dynamic & Static \\
725 type &GFLOPS & Freq. & Freq. & Freq. & power & power \\
726 & & GHz & GHz &GHz & & \\
728 1 &40 & 2.5 & 1.2 & 0.1 & 20~w &4~w \\
731 2 &50 & 2.66 & 1.6 & 0.133 & 25~w &5~w \\
734 3 &60 & 2.9 & 1.2 & 0.1 & 30~w &6~w \\
737 4 &70 & 3.4 & 1.6 & 0.133 & 35~w &7~w \\
741 \label{table:platform}
745 %\subsection{Performance prediction verification}
748 \subsection{The experimental results of the scaling algorithm}
752 The proposed algorithm was applied to the seven parallel NAS benchmarks (EP, CG,
753 MG, FT, BT, LU and SP) and the benchmarks were executed with the three classes:
754 A, B and C. However, due to the lack of space in this paper, only the results of
755 the biggest class, C, are presented while being run on different number of
756 nodes, ranging from 4 to 128 or 144 nodes depending on the benchmark being
757 executed. Indeed, the benchmarks CG, MG, LU, EP and FT had to be executed on $1,
758 2, 4, 8, 16, 32, 64, 128$ nodes. The other benchmarks such as BT and SP had to
759 be executed on $1, 4, 9, 16, 36, 64, 144$ nodes.
764 \caption{Running NAS benchmarks on 4 nodes }
767 \begin{tabular}{|*{7}{l|}}
769 Program & Execution & Energy & Energy & Performance & Distance \\
770 name & time/s & consumption/J & saving\% & degradation\% & \\
772 CG & 64.64 & 3560.39 &34.16 &6.72 &27.44 \\
774 MG & 18.89 & 1074.87 &35.37 &4.34 &31.03 \\
776 EP &79.73 &5521.04 &26.83 &3.04 &23.79 \\
778 LU &308.65 &21126.00 &34.00 &6.16 &27.84 \\
780 BT &360.12 &21505.55 &35.36 &8.49 &26.87 \\
782 SP &234.24 &13572.16 &35.22 &5.70 &29.52 \\
784 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}{l|}}
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 \\
818 \caption{Running NAS benchmarks on 16 nodes }
821 \begin{tabular}{|*{7}{l|}}
823 Program & Execution & Energy & Energy & Performance & Distance \\
824 name & time/s & consumption/J & saving\% & degradation\% & \\
826 CG &31.74 &4373.90 &26.29 &9.57 &16.72 \\
828 MG &5.71 &1076.19 &32.49 &6.05 &26.44 \\
830 EP &20.11 &5638.49 &26.85 &0.56 &26.29 \\
832 LU &144.13 &42529.06 &28.80 &6.56 &22.24 \\
834 BT &97.29 &22813.86 &34.95 &5.80 &29.15 \\
836 SP &66.49 &20821.67 &22.49 &3.82 &18.67 \\
838 FT &37.01 &5505.60 &31.59 &6.48 &25.11 \\
841 \label{table:res_16n}
845 \caption{Running NAS benchmarks on 32 and 36 nodes }
848 \begin{tabular}{|*{7}{l|}}
850 Program & Execution & Energy & Energy & Performance & Distance \\
851 name & time/s & consumption/J & saving\% & degradation\% & \\
853 CG &32.35 &6704.21 &16.15 &5.30 &10.85 \\
855 MG &4.30 &1355.58 &28.93 &8.85 &20.08 \\
857 EP &9.96 &5519.68 &26.98 &0.02 &26.96 \\
859 LU &99.93 &67463.43 &23.60 &2.45 &21.15 \\
861 BT &48.61 &23796.97 &34.62 &5.83 &28.79 \\
863 SP &46.01 &27007.43 &22.72 &3.45 &19.27 \\
865 FT &28.06 &7142.69 &23.09 &2.90 &20.19 \\
868 \label{table:res_32n}
872 \caption{Running NAS benchmarks on 64 nodes }
875 \begin{tabular}{|*{7}{l|}}
877 Program & Execution & Energy & Energy & Performance & Distance \\
878 name & time/s & consumption/J & saving\% & degradation\% & \\
880 CG &46.65 &17521.83 &8.13 &1.68 &6.45 \\
882 MG &3.27 &1534.70 &29.27 &14.35 &14.92 \\
884 EP &5.05 &5471.1084 &27.12 &3.11 &24.01 \\
886 LU &73.92 &101339.16 &21.96 &3.67 &18.29 \\
888 BT &39.99 &27166.71 &32.02 &12.28 &19.74 \\
890 SP &52.00 &49099.28 &24.84 &0.03 &24.81 \\
892 FT &25.97 &10416.82 &20.15 &4.87 &15.28 \\
895 \label{table:res_64n}
900 \caption{Running NAS benchmarks on 128 and 144 nodes }
903 \begin{tabular}{|*{7}{l|}}
905 Program & Execution & Energy & Energy & Performance & Distance \\
906 name & time/s & consumption/J & saving\% & degradation\% & \\
908 CG &56.92 &41163.36 &4.00 &1.10 &2.90 \\
910 MG &3.55 &2843.33 &18.77 &10.38 &8.39 \\
912 EP &2.67 &5669.66 &27.09 &0.03 &27.06 \\
914 LU &51.23 &144471.90 &16.67 &2.36 &14.31 \\
916 BT &37.96 &44243.82 &23.18 &1.28 &21.90 \\
918 SP &64.53 &115409.71 &26.72 &0.05 &26.67 \\
920 FT &25.51 &18808.72 &12.85 &2.84 &10.01 \\
923 \label{table:res_128n}
925 The overall energy consumption was computed for each instance according to the
926 energy consumption model (\ref{eq:energy}), with and without applying the
927 algorithm. The execution time was also measured for all these experiments. Then,
928 the energy saving and performance degradation percentages were computed for each
929 instance. The results are presented in Tables (\ref{table:res_4n},
930 \ref{table:res_8n}, \ref{table:res_16n}, \ref{table:res_32n},
931 \ref{table:res_64n} and \ref{table:res_128n}). All these results are the average
932 values from many experiments for energy savings and performance degradation.
933 The tables show the experimental results for running the NAS parallel benchmarks
934 on different number of nodes. The experiments show that the algorithm
935 significantly reduces the energy consumption (up to 35\%) and tries to limit the
936 performance degradation. They also show that the energy saving percentage
937 decreases when the number of computing nodes increases. This reduction is due
938 to the increase of the communication times compared to the execution times when
939 the benchmarks are run over a high number of nodes. Indeed, the benchmarks with
940 the same class, C, are executed on different numbers of nodes, so the
941 computation required for each iteration is divided by the number of computing
942 nodes. On the other hand, more communications are required when increasing the
943 number of nodes so the static energy increases linearly according to the
944 communication time and the dynamic power is less relevant in the overall energy
945 consumption. Therefore, reducing the frequency with algorithm~(\ref{HSA}) is
946 less effective in reducing the overall energy savings. It can also be noticed
947 that for the benchmarks EP and SP that contain little or no communications, the
948 energy savings are not significantly affected by the high number of nodes. No
949 experiments were conducted using bigger classes than D, because they require a
950 lot of memory (more than 64GB) when being executed by the simulator on one
951 machine. The maximum distance between the normalized energy curve and the
952 normalized performance for each instance is also shown in the result tables. It
953 decrease in the same way as the energy saving percentage. The tables also show
954 that the performance degradation percentage is not significantly increased when
955 the number of computing nodes is increased because the computation times are
956 small when compared to the communication times.
962 \subfloat[Energy saving]{%
963 \includegraphics[width=.33\textwidth]{fig/energy}\label{fig:energy}}%
965 \subfloat[Performance degradation ]{%
966 \includegraphics[width=.33\textwidth]{fig/per_deg}\label{fig:per_deg}}
968 \caption{The energy and performance for all NAS benchmarks running with a different number of nodes}
971 Figures \ref{fig:energy} and \ref{fig:per_deg} present the energy saving and
972 performance degradation respectively for all the benchmarks according to the
973 number of used nodes. As shown in the first plot, the energy saving percentages
974 of the benchmarks MG, LU, BT and FT decrease linearly when the number of nodes
975 increase. While for the EP and SP benchmarks, the energy saving percentage is
976 not affected by the increase of the number of computing nodes, because in these
977 benchmarks there are little or no communications. Finally, the energy saving of
978 the GC benchmark significantly decrease when the number of nodes increase
979 because this benchmark has more communications than the others. The second plot
980 shows that the performance degradation percentages of most of the benchmarks
981 decrease when they run on a big number of nodes because they spend more time
982 communicating than computing, thus, scaling down the frequencies of some nodes
983 has less effect on the performance.
988 \subsection{The results for different power consumption scenarios}
990 The results of the previous section were obtained while using processors that
991 consume during computation an overall power which is 80\% composed of dynamic
992 power and of 20\% of static power. In this section, these ratios are changed and
993 two new power scenarios are considered in order to evaluate how the proposed
994 algorithm adapts itself according to the static and dynamic power values. The
995 two new power scenarios are the following:
998 \item 70\% of dynamic power and 30\% of static power
999 \item 90\% of dynamic power and 10\% of static power
1002 The NAS parallel benchmarks were executed again over processors that follow the
1003 new power scenarios. The class C of each benchmark was run over 8 or 9 nodes
1004 and the results are presented in Tables \ref{table:res_s1} and
1005 \ref{table:res_s2}. These tables show that the energy saving percentage of the
1006 70\%-30\% scenario is smaller for all benchmarks compared to the energy saving
1007 of the 90\%-10\% scenario. Indeed, in the latter more dynamic power is consumed
1008 when nodes are running on their maximum frequencies, thus, scaling down the
1009 frequency of the nodes results in higher energy savings than in the 70\%-30\%
1010 scenario. On the other hand, the performance degradation percentage is smaller
1011 in the 70\%-30\% scenario compared to the 90\%-10\% scenario. This is due to the
1012 higher static power percentage in the first scenario which makes it more
1013 relevant in the overall consumed energy. Indeed, the static energy is related
1014 to the execution time and if the performance is degraded the amount of consumed
1015 static energy directly increas. Therefore, the proposed algorithm does not
1016 really significantly scale down much the frequencies of the nodes in order to
1017 limit the increase of the execution time and thus limiting the effect of the
1018 consumed static energy.
1020 Both new power scenarios are compared to the old one in figure
1021 (\ref{fig:sen_comp}). It shows the average of the performance degradation, the
1022 energy saving and the distances for all NAS benchmarks of class C running on 8
1023 or 9 nodes. The comparison shows that the energy saving ratio is proportional
1024 to the dynamic power ratio: it is increased when applying the 90\%-10\% scenario
1025 because at maximum frequency the dynamic energy is the most relevant in the
1026 overall consumed energy and can be reduced by lowering the frequency of some
1027 processors. On the other hand, the energy saving decreases when the 70\%-30\%
1028 scenario is used because the dynamic energy is less relevant in the overall
1029 consumed energy and lowering the frequency does not return big energy savings.
1030 Moreover, the average of the performance degradation is decreased when using a
1031 higher ratio for static power (e.g. 70\%-30\% scenario and 80\%-20\%
1032 scenario). Since the proposed algorithm optimizes the energy consumption when
1033 using a higher ratio for dynamic power the algorithm selects bigger frequency
1034 scaling factors that result in more energy saving but less performance, for
1035 example see Figure (\ref{fig:scales_comp}). The opposite happens when using a
1036 higher ratio for static power, the algorithm proportionally selects smaller
1037 scaling values which result in less energy saving but also less performance
1042 \caption{The results of the 70\%-30\% power scenario}
1045 \begin{tabular}{|*{6}{l|}}
1047 Program & Energy & Energy & Performance & Distance \\
1048 name & consumption/J & saving\% & degradation\% & \\
1050 CG &4144.21 &22.42 &7.72 &14.70 \\
1052 MG &1133.23 &24.50 &5.34 &19.16 \\
1054 EP &6170.30 &16.19 &0.02 &16.17 \\
1056 LU &39477.28 &20.43 &0.07 &20.36 \\
1058 BT &26169.55 &25.34 &6.62 &18.71 \\
1060 SP &19620.09 &19.32 &3.66 &15.66 \\
1062 FT &6094.07 &23.17 &0.36 &22.81 \\
1065 \label{table:res_s1}
1071 \caption{The results of the 90\%-10\% power scenario}
1074 \begin{tabular}{|*{6}{l|}}
1076 Program & Energy & Energy & Performance & Distance \\
1077 name & consumption/J & saving\% & degradation\% & \\
1079 CG &2812.38 &36.36 &6.80 &29.56 \\
1081 MG &825.427 &38.35 &6.41 &31.94 \\
1083 EP &5281.62 &35.02 &2.68 &32.34 \\
1085 LU &31611.28 &39.15 &3.51 &35.64 \\
1087 BT &21296.46 &36.70 &6.60 &30.10 \\
1089 SP &15183.42 &35.19 &11.76 &23.43 \\
1091 FT &3856.54 &40.80 &5.67 &35.13 \\
1094 \label{table:res_s2}
1100 \subfloat[Comparison between the results on 8 nodes]{%
1101 \includegraphics[width=.33\textwidth]{fig/sen_comp}\label{fig:sen_comp}}%
1103 \subfloat[Comparison the selected frequency scaling factors of MG benchmark class C running on 8 nodes]{%
1104 \includegraphics[width=.33\textwidth]{fig/three_scenarios}\label{fig:scales_comp}}
1106 \caption{The comparison of the three power scenarios}
1112 \subsection{The comparison of the proposed scaling algorithm }
1113 \label{sec.compare_EDP}
1114 In this section, the scaling factors selection algorithm, called MaxDist,
1115 is compared to Spiliopoulos et al. algorithm \cite{Spiliopoulos_Green.governors.Adaptive.DVFS}, called EDP.
1116 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, $EDP=Enegry*Delay$ using the predicted overall energy consumption and execution time delay for each frequency.
1117 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
1118 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.
1120 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 consumptions 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,
1121 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\%.
1124 For all benchmarks, our algorithm outperforms Spiliopoulos et al. algorithm in
1125 terms of energy and performance tradeoff, see figure (\ref{fig:compare_EDP}),
1126 because it maximizes the distance between the energy saving and the performance
1127 degradation values while giving the same weight for both metrics.
1133 \caption{Comparing the proposed algorithm}
1135 \begin{tabular}{|l|l|l|l|l|l|l|l|}
1137 \multicolumn{2}{|l|}{\multirow{2}{*}{\begin{tabular}[c]{@{}l@{}}Program \\ name\end{tabular}}} & \multicolumn{2}{l|}{Energy saving \%} & \multicolumn{2}{l|}{Perf. degradation \%} & \multicolumn{2}{l|}{Distance} \\ \cline{3-8}
1138 \multicolumn{2}{|l|}{} & EDP & MaxDist & EDP & MaxDist & EDP & MaxDist \\ \hline
1139 \multicolumn{2}{|l|}{CG} & 27.58 & 31.25 & 5.82 & 7.12 & 21.76 & 24.13 \\ \hline
1140 \multicolumn{2}{|l|}{MG} & 29.49 & 33.78 & 3.74 & 6.41 & 25.75 & 27.37 \\ \hline
1141 \multicolumn{2}{|l|}{LU} & 19.55 & 28.33 & 0.0 & 0.01 & 19.55 & 28.22 \\ \hline
1142 \multicolumn{2}{|l|}{EP} & 28.40 & 27.04 & 4.29 & 0.49 & 24.11 & 26.55 \\ \hline
1143 \multicolumn{2}{|l|}{BT} & 27.68 & 32.32 & 6.45 & 7.87 & 21.23 & 24.43 \\ \hline
1144 \multicolumn{2}{|l|}{SP} & 20.52 & 24.73 & 5.21 & 2.78 & 15.31 & 21.95 \\ \hline
1145 \multicolumn{2}{|l|}{FT} & 27.03 & 31.02 & 2.75 & 2.54 & 24.28 & 28.48 \\ \hline
1148 \label{table:compare_EDP}
1157 \includegraphics[scale=0.5]{fig/compare_EDP.pdf}
1158 \caption{Tradeoff comparison for NAS benchmarks class C}
1159 \label{fig:compare_EDP}
1163 \section{Conclusion}
1165 In this paper, a new online frequency selecting algorithm has been presented. It
1166 selects the best possible vector of frequency scaling factors that gives the
1167 maximum distance (optimal tradeoff) between the predicted energy and the
1168 predicted performance curves for a heterogeneous platform. This algorithm uses a
1169 new energy model for measuring and predicting the energy of distributed
1170 iterative applications running over heterogeneous platforms. To evaluate the
1171 proposed method, it was applied on the NAS parallel benchmarks and executed over
1172 a heterogeneous platform simulated by Simgrid. The results of the experiments
1173 showed that the algorithm reduces up to 35\% the energy consumption of a message
1174 passing iterative method while limiting the degradation of the performance. The
1175 algorithm also selects different scaling factors according to the percentage of
1176 the computing and communication times, and according to the values of the static
1177 and dynamic powers of the CPUs. Finally, the algorithm was compared to
1178 Spiliopoulos et al. algorithm and the results showed that it outperforms their
1179 algorithm in terms of energy-time tradeoff.
1181 In the near future, this method will be applied to real heterogeneous platforms
1182 to evaluate its performance in a real study case. It would also be interesting
1183 to evaluate its scalability over large scale heterogeneous platforms and measure
1184 the energy consumption reduction it can produce. Afterward, we would like to
1185 develop a similar method that is adapted to asynchronous iterative applications
1186 where each task does not wait for other tasks to finish their works. The
1187 development of such a method might require a new energy model because the number
1188 of iterations is not known in advance and depends on the global convergence of
1189 the iterative system.
1191 \section*{Acknowledgment}
1193 This work has been partially supported by the Labex
1194 ACTION project (contract “ANR-11-LABX-01-01”). As a PhD student,
1195 Mr. Ahmed Fanfakh, would like to thank the University of
1196 Babylon (Iraq) for supporting his work.
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1209 %%% Local Variables:
1213 %%% ispell-local-dictionary: "american"
1216 % LocalWords: Fanfakh Charr FIXME Tianhe DVFS HPC NAS NPB SMPI Rauber's Rauber
1217 % LocalWords: CMOS EPSA Franche Comté Tflop Rünger IUT Maréchal Juin cedex
1218 % LocalWords: de badri muslim MPI TcpOld TcmOld dNew dOld cp Sopt Tcp Tcm Ps
1219 % LocalWords: Scp Fmax Fdiff SimGrid GFlops Xeon EP BT