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56 \title{Energy Consumption Reduction in heterogeneous architecture using DVFS}
67 University of Franche-Comté\\
68 IUT de Belfort-Montbéliard,
69 19 avenue du Maréchal Juin, BP 527, 90016 Belfort cedex, France\\
70 % Telephone: \mbox{+33 3 84 58 77 86}, % Raphaël
71 % Fax: \mbox{+33 3 84 58 77 81}\\ % Dept Info
72 Email: \email{{jean-claude.charr,raphael.couturier,ahmed.fanfakh_badri_muslim,arnaud.giersch}@univ-fcomte.fr}
82 \section{Introduction}
86 \section{Related works}
93 \section{The performance and energy consumption measurements on heterogeneous architecture}
96 % \JC{The whole subsection ``Parallel Tasks Execution on Homogeneous Platform'',
97 % can be deleted if we need space, we can just say we are interested in this
98 % paper in homogeneous clusters}
100 \subsection{The execution time of message passing distributed iterative applications on a heterogeneous platform}
102 In this paper, we are interested in reducing the energy consumption of message
103 passing distributed iterative synchronous applications running over
104 heterogeneous platforms. We define a heterogeneous platform as a collection of
105 heterogeneous computing nodes interconnected via a high speed homogeneous
106 network. Therefore, each node has different characteristics such as computing
107 power (FLOPS), energy consumption, CPU's frequency range, ... but they all have
108 the same network bandwidth and latency.
113 \includegraphics[scale=0.6]{fig/commtasks}
114 \caption{Parallel tasks on a heterogeneous platform}
118 The overall execution time of a distributed iterative synchronous application over a heterogeneous platform consists of the sum of the computation time and the communication time for every iteration on a node. However, due to the heterogeneous computation power of the computing nodes, slack times might occur when fast nodes have to
119 wait, during synchronous communications, for the slower nodes to finish their computations (see Figure~(\ref{fig:heter})).
120 Therefore, the overall execution time of the program is the execution time of the slowest
121 task which have the highest computation time and no slack time.
123 Dynamic Voltage and Frequency Scaling (DVFS) is a process, implemented in modern processors, that reduces the energy consumption
124 of a CPU by scaling down its voltage and frequency. Since DVFS lowers the frequency of a CPU and consequently its computing power, the execution time of a program running over that scaled down processor might increase, especially if the program is compute bound. The frequency reduction process can be expressed by the scaling factor S which is the ratio between the maximum and the new frequency of a CPU as in EQ (\ref{eq:s}).
127 S = \frac{F_\textit{max}}{F_\textit{new}}
129 The execution time of a compute bound sequential program is linearly proportional to the frequency scaling factor $S$.
130 On the other hand, message passing distributed applications consist of two parts: computation and communication. The execution time of the computation part is linearly proportional to the frequency scaling factor $S$ but the communication time is not affected by the scaling factor because the processors involved remain idle during the communications~\cite{17}. The communication time for a task is the summation of periods of time that begin with an MPI call for sending or receiving a message till the message is synchronously sent or received.
132 Since in a heterogeneous platform, each node has different characteristics, especially different frequency gears, when applying DVFS operations on these nodes, they may get different scaling factors represented by a scaling vector: $(S_1, S_2,..., S_N)$ where $S_i$ is the scaling factor of processor $i$. To be able to predict the execution time of message passing synchronous iterative applications running over a heterogeneous platform, for different vectors of scaling factors, the communication time and the computation time for all the
133 tasks must be measured during the first iteration before applying any DVFS operation. Then the execution time for one iteration of the application with any vector of scaling factors can be predicted using EQ (\ref{eq:perf}).
139 \textit T_\textit{new} =
140 {} \max_{i=1,2,\dots,N} (TcpOld_{i} \cdot S_{i}) + TcmOld_{j}
142 where $TcpOld_i$ is the computation time of processor $i$ during the first iteration and $TcmOld_j$ is the communication time of the slowest processor $j$.
143 The model computes the maximum computation time
144 with scaling factor from each node added to the communication time of the slowest node, it means only the
145 communication time without any slack time.
147 This prediction model is based on our model for predicting the execution time of message passing distributed applications for homogeneous architectures~\cite{45}. The execution time prediction model is used in our method for optimizing both energy consumption and performance of iterative methods, which is presented in the following sections.
150 \subsection{Energy model for heterogeneous platform}
152 Many researchers~\cite{9,3,15,26} divide the power consumed by a processor into
153 two power metrics: the static and the dynamic power. While the first one is
154 consumed as long as the computing unit is turned on, the latter is only consumed during
155 computation times. The dynamic power $P_{d}$ is related to the switching
156 activity $\alpha$, load capacitance $C_L$, the supply voltage $V$ and
157 operational frequency $F$, as shown in EQ(\ref{eq:pd}).
160 P_\textit{d} = \alpha \cdot C_L \cdot V^2 \cdot F
162 The static power $P_{s}$ captures the leakage power as follows:
165 P_\textit{s} = V \cdot N_{trans} \cdot K_{design} \cdot I_{leak}
167 where V is the supply voltage, $N_{trans}$ is the number of transistors,
168 $K_{design}$ is a design dependent parameter and $I_{leak}$ is a
169 technology-dependent parameter. The energy consumed by an individual processor
170 to execute a given program can be computed as:
173 E_\textit{ind} = P_\textit{d} \cdot T_{cp} + P_\textit{s} \cdot T
175 where $T$ is the execution time of the program, $T_{cp}$ is the computation
176 time and $T_{cp} \leq T$. $T_{cp}$ may be equal to $T$ if there is no
177 communication and no slack time.
179 The main objective of DVFS operation is to
180 reduce the overall energy consumption~\cite{37}. The operational frequency $F$
181 depends linearly on the supply voltage $V$, i.e., $V = \beta \cdot F$ with some
182 constant $\beta$. This equation is used to study the change of the dynamic
183 voltage with respect to various frequency values in~\cite{3}. The reduction
184 process of the frequency can be expressed by the scaling factor $S$ which is the
185 ratio between the maximum and the new frequency as in EQ~(\ref{eq:s}).
186 The CPU governors are power schemes supplied by the operating
187 system's kernel to lower a core's frequency. we can calculate the new frequency
188 $F_{new}$ from EQ(\ref{eq:s}) as follow:
191 F_\textit{new} = S^{-1} . F_\textit{max}
193 Replacing $F_{new}$ in EQ(\ref{eq:pd}) as in EQ(\ref{eq:fnew}) gives the following equation for dynamic
197 {P}_\textit{dNew} = \alpha \cdot C_L \cdot V^2 \cdot F_{new} = \alpha \cdot C_L \cdot \beta^2 \cdot F_{new}^3 \\
198 = \alpha \cdot C_L \cdot V^2 \cdot F \cdot S^{-3} = P_{dOld} \cdot S^{-3}
200 where $ {P}_\textit{dNew}$ and $P_{dOld}$ are the dynamic power consumed with the new frequency and the maximum frequency respectively.
202 According to EQ(\ref{eq:pdnew}) the dynamic power is reduced by a factor of $S^{-3}$ when
203 reducing the frequency by a factor of $S$~\cite{3}. Since the FLOPS of a CPU is proportional to the frequency of a CPU, the computation time is increased proportionally to $S$. The new dynamic energy is the dynamic power multiplied by the new time of computation and is given by the following equation:
206 E_\textit{dNew} = P_{dOld} \cdot S^{-3} \cdot (T_{cp} \cdot S)= S^{-2}\cdot P_{dOld} \cdot T_{cp}
208 The static power is related to the power leakage of the CPU and is consumed during computation and even when idle. As in~\cite{3,46}, we assume that the static power of a processor is constant during idle and computation periods, and for all its available frequencies.
209 The static energy is the static power multiplied by the execution time of the program. According to the execution time model in EQ(\ref{eq:perf}),
210 the execution time of the program is the summation of the computation and the communication times. The computation time is linearly related
211 to the frequency scaling factor, while this scaling factor does not affect the communication time. The static energy
212 of a processor after scaling its frequency is computed as follows:
216 E_\textit{s} = P_\textit{s} \cdot (T_{cp} \cdot S + T_{cm})
219 In the considered heterogeneous platform, each processor $i$ might have different dynamic and static powers, noted as $P_{di}$ and $P_{si}$ respectively. Therefore, even if the distributed message passing iterative application is load balanced, the computation time of each CPU $i$ noted $T_{cpi}$ might be different and different frequency scaling factors might be computed in order to decrease the overall energy consumption of the application and reduce the slack times. The communication time of a processor $i$ is noted as $T_{cmi}$ and could contain slack times if it is communicating with slower nodes, see figure(\ref{fig:heter}). Therefore, all nodes do not have equal communication times. While the dynamic energy is computed according to the frequency scaling factor and the dynamic power of each node as in EQ(\ref{eq:Edyn}), the static energy is computed as the sum of the execution time of each processor multiplied by its static power. The overall energy consumption of a message passing distributed application executed over a heterogeneous platform is the summation of all dynamic and static energies for each processor. It is computed as follows:
222 E = \sum_{i=1}^{N} {(S_i^{-2} \cdot P_{di} \cdot T_{cpi})} +\\
223 {}\sum_{i=1}^{N} {(P_{si} \cdot (\max_{i=1,2,\dots,N} (T_{cpi} \cdot S_{i}) +}
224 {}\min_{i=1,2,\dots,N} {T_{cmi}))}
227 Reducing the the frequencies of the processors according to the vector of scaling factors $(S_1, S_2,..., S_N)$ may degrade the performance of the application and thus,
228 increase the static energy because the execution time is increased~\cite{36}.
230 \section{Optimization of both energy consumption and performance}
232 Applying DVFS to lower level not surly reducing the energy consumption to minimum level. Also, a big scaling for the frequency produces high performance degradation percent. Moreover, by considering the drastically increase in execution time of parallel program, the static energy is related to this time
233 and it also increased by the same ratio. Thus, the opportunity for gaining more energy reduction is restricted. For that choosing frequency scaling factors is very important process to taking into account both energy and performance. In our previous work~\cite{45}, we are proposed a method that selects the optimal frequency scaling factor for an homogeneous cluster, depending on the trade-off relation between the energy and performance. In this work we have an heterogeneous cluster, at each node there is different scaling factors, so our goal is to selects the optimal set of frequency scaling factors, $Sopt_1,Sopt_2,...,Sopt_N$, that gives the best trade-off between energy consumption and performance. The relation between the energy and the execution time is complex and nonlinear, Thus, unlike the relation between the performance and the scaling factor, the relation of the energy with the frequency scaling factors is nonlinear, for more details refer to~\cite{17}. Moreover, they are not measured using the same metric. To solve this problem, we normalize the execution time by calculating the ratio between the new execution time (the scaled execution time) and the old one as follow:
236 P_\textit{Norm} = \frac{T_\textit{New}}{T_\textit{Old}}\\
237 = \frac{ \max_{i=1,2,\dots,N} (Tcp_{i} \cdot S_{i}) +\min_{i=1,2,\dots,N} {Tcm_{i}}}
238 {\max_{i=1,2,\dots,N}{(Tcp_i+Tcm_i)}}
242 By the same way, we are normalize the energy by calculating the ratio between the consumed energy with scaled frequency and the consumed energy without scaled frequency:
245 E_\textit{Norm} = \frac{E_\textit{Reduced}}{E_\textit{Original}} \\
246 = \frac{ \sum_{i=1}^{N}{(S_i^{-2} \cdot Pd_i \cdot Tcp_i)} +
247 \sum_{i=1}^{N} {(Ps_i \cdot T_{New})}}{\sum_{i=1}^{N}{( Pd_i \cdot Tcp_i)} +
248 \sum_{i=1}^{N} {(Ps_i \cdot T_{Old})}}
250 Where $T_{New}$ and $T_{Old}$ is computed as in EQ(\ref{eq:pnorm}). The second problem
251 is that the optimization operation for both energy and performance is not in the same direction.
252 In other words, the normalized energy and the normalized execution time curves are not at the same direction.
253 While the main goal is to optimize the energy and execution time in the same time. According to the
254 equations~(\ref{eq:enorm}) and~(\ref{eq:pnorm}), the set of frequency scaling factors $S_1,S_2,...,S_N$ reduce both the energy and the
255 execution time simultaneously. But the main objective is to produce maximum energy
256 reduction with minimum execution time reduction. Many researchers used different
257 strategies to solve this nonlinear problem for example see~\cite{19,42}, their
258 methods add big overheads to the algorithm to select the suitable frequency.
259 In this paper we are present a method to find the optimal set of frequency scaling factors to optimize both energy and execution time simultaneously
260 without adding a big overhead. Our solution for this problem is to make the optimization process
261 for energy and execution time follow the same direction. Therefore, we inverse the equation of the normalized
262 execution time, the normalized performance, as follows:
266 P_\textit{Norm} = \frac{T_\textit{Old}}{T_\textit{New}}\\
267 = \frac{\max_{i=1,2,\dots,N}{(Tcp_i+Tcm_i)}}
268 { \max_{i=1,2,\dots,N} (Tcp_{i} \cdot S_{i}) +\min_{i=1,2,\dots,N} {Tcm_{i}}}
274 \subfloat[Homogeneous platform]{%
275 \includegraphics[width=.22\textwidth]{fig/homo}\label{fig:r1}}%
277 \subfloat[Heterogeneous platform]{%
278 \includegraphics[width=.22\textwidth]{fig/heter}\label{fig:r2}}
280 \caption{The energy and performance relation}
283 Then, we can model our objective function as finding the maximum distance
284 between the energy curve EQ~(\ref{eq:enorm}) and the performance
285 curve EQ~(\ref{eq:pnorm_inv}) over all available sets of scaling factors. This
286 represents the minimum energy consumption with minimum execution time (better
287 performance) at the same time, see figure~(\ref{fig:r1}) or figure~(\ref{fig:r2}) . Then our objective
288 function has the following form:
292 \max_{i=1,\dots F, j=1,\dots,N}
293 (\overbrace{P_\textit{Norm}(S_{ij})}^{\text{Maximize}} -
294 \overbrace{E_\textit{Norm}(S_{ij})}^{\text{Minimize}} )
296 where $N$ is the number of nodes and $F$ is the number of available frequencies for each nodes.
297 Then we can select the optimal set of scaling factors that satisfies EQ~(\ref{eq:max}). Our objective function can
298 work with any energy model or energy values stored in a data file.
299 Moreover, this function works in optimal way when the energy curve has a convex
300 form over the available frequency scaling factors as shown in~\cite{15,3,19}.
302 \section{The heterogeneous scaling algorithm }
305 In this section we proposed an heterogeneous scaling algorithm,
306 (figure~\ref{HSA}), that selects the optimal set of scaling factors from each
307 node. The algorithm is numerates the suitable range of available scaling
308 factors for each node in the heterogeneous cluster, returns a set of optimal
309 frequency scaling factors for each node. Using heterogeneous cluster is produces
310 different workloads for each node. Therefore, the fastest nodes waiting at the
311 barrier for the slowest nodes to finish there work as in figure
312 (\ref{fig:heter}). Our algorithm takes into account these imbalanced workloads
313 when is starts to search for selecting the best scaling factors. So, the
314 algorithm is selecting the initial frequencies values for each node proportional
315 to the times of computations that gathered from the first iteration. As an
316 example in figure (\ref{fig:st_freq}), the algorithm don't test the first
317 frequencies of the fastest nodes until it converge their frequencies to the
318 frequency of the slowest node. If the algorithm is starts test changing the
319 frequency of the slowest nodes from beginning, we are loosing performance and
320 then not selecting the best trade-off (the distance). This case will be similar
321 to the homogeneous cluster when all nodes scales their frequencies together from
322 the beginning. In this case there is a small distance between energy and
323 performance curves, for example see the figure(\ref{fig:r1}). Then the
324 algorithm searching for optimal frequency scaling factor from the selected
325 frequencies until the last available ones.
328 \includegraphics[scale=0.5]{fig/start_freq}
329 \caption{Selecting the initial frequencies}
334 To compute the initial frequencies, the algorithm firstly needs to compute the computation scaling factors $Scp_i$ for each node. Each one of these factors represent a ratio between the computation time of the slowest node and the computation time of the node $i$ as follow:
337 Scp_{i} = \frac{\max_{i=1,2,\dots,N}(Tcp_i)}{Tcp_i}
339 Depending on the initial computation scaling factors EQ(\ref{eq:Scp}), the algorithm computes the initial frequencies for all nodes as a ratio between the
340 maximum frequency of node $i$ and the computation scaling factor $Scp_i$ as follow:
343 F_{i} = \frac{Fmax_i}{Scp_i},~{i=1,2,\cdots,N}
346 \begin{algorithmic}[1]
350 \item[$Tcp_i$] array of all computation times for all nodes during one iteration and with highest frequency.
351 \item[$Tcm_i$] array of all communication times for all nodes during one iteration and with highest frequency.
352 \item[$Fmax_i$] array of the maximum frequencies for all nodes.
353 \item[$Pd_i$] array of the dynamic powers for all nodes.
354 \item[$Ps_i$] array of the static powers for all nodes.
355 \item[$Fdiff_i$] array of the difference between two successive frequencies for all nodes.
357 \Ensure $Sopt_1, \dots ,Sopt_N$ is a set of optimal scaling factors
359 \State $ Scp_i \gets \frac{\max_{i=1,2,\dots,N}(Tcp_i)}{Tcp_i} $
360 \State $F_{i} \gets \frac{Fmax_i}{Scp_i},~{i=1,2,\cdots,N}$
361 \State Round the computed initial frequencies $F_i$ to the closest one available in each node.
362 \If{(not the first frequency)}
363 \State $F_i \gets F_i+Fdiff_i,~i=1,...,N.$
365 \State $T_\textit{Old} \gets max_{~i=1,...,N } (Tcp_i+Tcm_i)$
366 \State $E_\textit{Original} \gets \sum_{i=1}^{N}{( Pd_i \cdot Tcp_i)} +\sum_{i=1}^{N} {(Ps_i \cdot T_{Old})}$
367 \State $Dist \gets 0$
368 \State $Sopt_{i} \gets 1,~i=1,...,N. $
369 \While {(all nodes not reach their minimum frequency)}
370 \If{(not the last freq. \textbf{and} not the slowest node)}
371 \State $F_i \gets F_i - Fdiff_i,~i=1,...,N.$
372 \State $S_i \gets \frac{Fmax_i}{F_i},~i=1,...,N.$
374 \State $T_{New} \gets max_\textit{~i=1,\dots,N} (Tcp_{i} \cdot S_{i}) + min_\textit{~i=1,\dots,N}(Tcm_i) $
375 \State $E_\textit{Reduced} \gets \sum_{i=1}^{N}{(S_i^{-2} \cdot Pd_i \cdot Tcp_i)} + $ \hspace*{43 mm}
376 $\sum_{i=1}^{N} {(Ps_i \cdot T_{New})} $
377 \State $ P_\textit{Norm} \gets \frac{T_\textit{Old}}{T_\textit{New}}$
378 \State $E_\textit{Norm}\gets \frac{E_\textit{Reduced}}{E_\textit{Original}}$
379 \If{$(\Pnorm - \Enorm > \Dist)$}
380 \State $Sopt_{i} \gets S_{i},~i=1,...,N. $
381 \State $\Dist \gets \Pnorm - \Enorm$
384 \State Return $Sopt_1,Sopt_2, \dots ,Sopt_N$
386 \caption{Heterogeneous scaling algorithm}
389 When the initial frequencies are computed the algorithm numerates all available
390 scaling factors starting from these frequencies until all nodes reach their
391 minimum frequencies. At each iteration the algorithm remains the frequency of
392 the slowest node without change and scaling the frequency of the other
393 nodes. This is gives better performance and energy trade-off. The proposed
394 algorithm works online during the execution time of the MPI program. Its
395 returns a set of optimal frequency scaling factors $Sopt_i$ depending on the
396 objective function EQ(\ref{eq:max}). The program changes the new frequencies of
397 the CPUs according to the computed scaling factors. This algorithm has a small
398 execution time: for an heterogeneous cluster composed of four different types of
399 nodes having the characteristics presented in table~(\ref{table:platform}), it
400 takes \np[ms]{0.04} on average for 4 nodes and \np[ms]{0.1} on average for 128
401 nodes. The algorithm complexity is $O(F\cdot (N \cdot4) )$, where $F$ is the
402 number of iterations and $N$ is the number of computing nodes. The algorithm
403 needs on average from 12 to 20 iterations for all the NAS benchmark on class C
404 to selects the best set of frequency scaling factors. Its called just once
405 during the execution of the program. The DVFS figure~(\ref{dvfs}) shows where
406 and when the algorithm is called in the MPI program.
408 \begin{algorithmic}[1]
410 \For {$k=1$ to \textit{some iterations}}
411 \State Computations section.
412 \State Communications section.
414 \State Gather all times of computation and\newline\hspace*{3em}%
415 communication from each node.
416 \State Call algorithm from Figure~\ref{HSA} with these times.
417 \State Compute the new frequencies from the\newline\hspace*{3em}%
418 returned optimal scaling factors.
419 \State Set the new frequencies to nodes.
423 \caption{DVFS algorithm}
427 \section{Experimental results}
430 The experiments of this work are executed on the simulator SimGrid/SMPI
431 v3.10~\cite{casanova+giersch+legrand+al.2014.versatile}. We configure the
432 simulator to use a heterogeneous cluster with one core per node. The proposed
433 heterogeneous cluster has four different types of nodes. Each node in cluster
434 has different characteristics such as the maximum frequency speed, the number of
435 available frequencies and dynamic and static powers values, see table
436 (\ref{table:platform}). These different types of processing nodes simulate some
437 real Intel processors. The maximum number of nodes that supported by the cluster
438 is 144 nodes according to characteristics of some MPI programs of the NAS
439 benchmarks that used. We are use the same number from each type of nodes when
440 running the MPI programs, for example if we execute the program on 8 node, there
441 are 2 nodes from each type participating in the computing. The dynamic and
442 static power values is different from one type to other. Each node has a dynamic
443 and static power values proportional to their performance/GFlops, for more
444 details see the Intel data sheets in \cite{47}. Each node has a percentage of
445 80\% for dynamic power and 20\% for static power from the hole power
446 consumption, the same assumption is made in \cite{45,3}. These nodes are
447 connected via an Ethernet network with 1 Gbit/s bandwidth.
449 \caption{Heterogeneous nodes characteristics}
452 \begin{tabular}{|*{7}{l|}}
454 Node & Similar & Max & Min & Diff. & Dynamic & Static \\
455 type & to & Freq. GHz & Freq. GHz & Freq GHz & power & power \\
457 1 & core-i3 & 2.5 & 1.2 & 0.1 & 20~w &4~w \\
460 2 & Xeon & 2.66 & 1.6 & 0.133 & 25~w &5~w \\
463 3 & core-i5 & 2.9 & 1.2 & 0.1 & 30~w &6~w \\
466 4 & core-i7 & 3.4 & 1.6 & 0.133 & 35~w &7~w \\
470 \label{table:platform}
474 %\subsection{Performance prediction verification}
477 \subsection{The experimental results of the scaling algorithm}
480 The proposed algorithm was applied to seven MPI programs of the NAS benchmarks (EP, CG, MG, FT, BT, LU and SP) NPB v3.
481 \cite{44}, which were run with three classes (A, B and C).
482 In this experiments we are focus on running of the class C, the biggest class compared to A and B, on different number of
483 nodes, from 4 to 128 or 144 nodes according to the type of the MPI program. Depending on the proposed energy consumption model EQ(\ref{eq:energy}),
484 we are measure the energy consumption for all NAS MPI programs. The dynamic and static power values used under the same assumption used by \cite{45,3}. We used a percentage of 80\% for dynamic power from all power consumption of the CPU and 20\% for static power. The heterogeneous nodes in table (\ref{table:platform}) have different simulated performance, ranked from the node of type 1 with smaller performance/GFlops to the highest performance/GFlops for node 4. Therefore, the power values used proportionally increased from node 1 to node 4 that with highest performance. Then we used an assumption that the power consumption increases linearly with the performance/GFlops of the processor see \cite{48}.
487 \caption{Running NAS benchmarks on 4 nodes }
490 \begin{tabular}{|*{7}{l|}}
492 Method & Execution & Energy & Energy & Performance & Distance \\
493 name & time/s & consumption/J & saving\% & degradation\% & \\
495 CG & 64.64 & 3560.39 &34.16 &6.72 &27.44 \\
497 MG & 18.89 & 1074.87 &35.37 &4.34 &31.03 \\
499 EP &79.73 &5521.04 &26.83 &3.04 &23.79 \\
501 LU &308.65 &21126.00 &34.00 &6.16 &27.84 \\
503 BT &360.12 &21505.55 &35.36 &8.49 &26.87 \\
505 SP &234.24 &13572.16 &35.22 &5.70 &29.52 \\
507 FT &81.58 &4151.48 &35.58 &0.99 &34.59 \\
514 \caption{Running NAS benchmarks on 8 and 9 nodes }
517 \begin{tabular}{|*{7}{l|}}
519 Method & Execution & Energy & Energy & Performance & Distance \\
520 name & time/s & consumption/J & saving\% & degradation\% & \\
522 CG &36.11 &3263.49 &31.25 &7.12 &24.13 \\
524 MG &8.99 &953.39 &33.78 &6.41 &27.37 \\
526 EP &40.39 &5652.81 &27.04 &0.49 &26.55 \\
528 LU &218.79 &36149.77 &28.23 &0.01 &28.22 \\
530 BT &166.89 &23207.42 &32.32 &7.89 &24.43 \\
532 SP &104.73 &18414.62 &24.73 &2.78 &21.95 \\
534 FT &51.10 &4913.26 &31.02 &2.54 &28.48 \\
541 \caption{Running NAS benchmarks on 16 nodes }
544 \begin{tabular}{|*{7}{l|}}
546 Method & Execution & Energy & Energy & Performance & Distance \\
547 name & time/s & consumption/J & saving\% & degradation\% & \\
549 CG &31.74 &4373.90 &26.29 &9.57 &16.72 \\
551 MG &5.71 &1076.19 &32.49 &6.05 &26.44 \\
553 EP &20.11 &5638.49 &26.85 &0.56 &26.29 \\
555 LU &144.13 &42529.06 &28.80 &6.56 &22.24 \\
557 BT &97.29 &22813.86 &34.95 &5.80 &29.15 \\
559 SP &66.49 &20821.67 &22.49 &3.82 &18.67 \\
561 FT &37.01 &5505.60 &31.59 &6.48 &25.11 \\
564 \label{table:res_16n}
568 \caption{Running NAS benchmarks on 32 and 36 nodes }
571 \begin{tabular}{|*{7}{l|}}
573 Method & Execution & Energy & Energy & Performance & Distance \\
574 name & time/s & consumption/J & saving\% & degradation\% & \\
576 CG &32.35 &6704.21 &16.15 &5.30 &10.85 \\
578 MG &4.30 &1355.58 &28.93 &8.85 &20.08 \\
580 EP &9.96 &5519.68 &26.98 &0.02 &26.96 \\
582 LU &99.93 &67463.43 &23.60 &2.45 &21.15 \\
584 BT &48.61 &23796.97 &34.62 &5.83 &28.79 \\
586 SP &46.01 &27007.43 &22.72 &3.45 &19.27 \\
588 FT &28.06 &7142.69 &23.09 &2.90 &20.19 \\
591 \label{table:res_32n}
595 \caption{Running NAS benchmarks on 64 nodes }
598 \begin{tabular}{|*{7}{l|}}
600 Method & Execution & Energy & Energy & Performance & Distance \\
601 name & time/s & consumption/J & saving\% & degradation\% & \\
603 CG &46.65 &17521.83 &8.13 &1.68 &6.45 \\
605 MG &3.27 &1534.70 &29.27 &14.35 &14.92 \\
607 EP &5.05 &5471.1084 &27.12 &3.11 &24.01 \\
609 LU &73.92 &101339.16 &21.96 &3.67 &18.29 \\
611 BT &39.99 &27166.71 &32.02 &12.28 &19.74 \\
613 SP &52.00 &49099.28 &24.84 &0.03 &24.81 \\
615 FT &25.97 &10416.82 &20.15 &4.87 &15.28 \\
618 \label{table:res_64n}
623 \caption{Running NAS benchmarks on 128 and 144 nodes }
626 \begin{tabular}{|*{7}{l|}}
628 Method & Execution & Energy & Energy & Performance & Distance \\
629 name & time/s & consumption/J & saving\% & degradation\% & \\
631 CG &56.92 &41163.36 &4.00 &1.10 &2.90 \\
633 MG &3.55 &2843.33 &18.77 &10.38 &8.39 \\
635 EP &2.67 &5669.66 &27.09 &0.03 &27.06 \\
637 LU &51.23 &144471.90 &16.67 &2.36 &14.31 \\
639 BT &37.96 &44243.82 &23.18 &1.28 &21.90 \\
641 SP &64.53 &115409.71 &26.72 &0.05 &26.67 \\
643 FT &25.51 &18808.72 &12.85 &2.84 &10.01 \\
646 \label{table:res_128n}
649 The results of applying the proposed scaling algorithm to NAS benchmarks is demonstrated in tables (\ref{table:res_4n}, \ref{table:res_8n}, \ref{table:res_16n},
650 \ref{table:res_32n}, \ref{table:res_64n} and \ref{table:res_128n}). These tables show the results for running the NAS benchmarks on different number of nodes. In general the energy saving percent is decreased when the number of the computing nodes is increased. While the distance is decreased by the same direction. This because when we are run the MPI programs on a big number of nodes the communications is biggest than the computations, so the static energy is increased linearly to these times. The tables also show that performance degradation percent still approximately the same or decreased a little when the number of computing nodes is increased. This gives good a prove that the proposed algorithm keeping as mush as possible the performance degradation.
654 \subfloat[Balanced nodes type scenario]{%
655 \includegraphics[width=.23185\textwidth]{fig/avg_eq}\label{fig:avg_eq}}%
657 \subfloat[Imbalanced nodes type scenario]{%
658 \includegraphics[width=.23185\textwidth]{fig/avg_neq}\label{fig:avg_neq}}
660 \caption{The average of energy and performance for all NAS benchmarks running with difference number of nodes}
663 In the NAS benchmarks there are some programs executed on different number of nodes. The benchmarks CG, MG, LU and FT executed on 2 to a power of (1, 2, 4, 8, ...) of nodes. The other benchmarks such as BT and SP executed on 2 to a power of (1, 2, 4, 9, ...) of nodes. We are take the average of energy saving, performance degradation and distances for all results of NAS benchmarks. The average of these three objectives are plotted to the number of nodes as in plots (\ref{fig:avg_eq} and \ref{fig:avg_neq}). In CG, MG, LU, and FT benchmarks the average of energy saving is decreased when the number of nodes is increased due to the increasing in the communication times as mentioned before. Thus, the average of distances (our objective function) is decreased linearly with energy saving while keeping the average of performance degradation the same. In BT and SP benchmarks, the average of energy saving is not decreased significantly compare to other benchmarks when the number of nodes is increased. Nevertheless, the average of performance degradation approximately still the same ratio. This difference is depends on the characteristics of the benchmarks such as the computation to communication ratio that has.
665 \subsection{The results for different powers scenarios}
667 The results of the previous section are obtained using a percentage of 80\% for
668 dynamic power and 20\% for static power of total power consumption. In this
669 section we are change these ratio by using two others scenarios. Because is
670 interested to measure the ability of the proposed algorithm to changes it
671 behavior when these power ratios are changed. In fact, we are use two different
672 scenarios for dynamic and static power ratios in addition to the previous
673 scenario in section (\ref{sec.res}). Therefore, we have three different
674 scenarios for three different dynamic and static power ratios refer to as:
675 70\%-20\%, 80\%-20\% and 90\%-10\% scenario. The results of these scenarios
676 running NAS benchmarks class C on 8 or 9 nodes are place in the tables
677 (\ref{table:res_s1} and \ref{table:res_s2}).
680 \caption{The results of 70\%-30\% powers scenario}
683 \begin{tabular}{|*{6}{l|}}
685 Method & Energy & Energy & Performance & Distance \\
686 name & consumption/J & saving\% & degradation\% & \\
688 CG &4144.21 &22.42 &7.72 &14.70 \\
690 MG &1133.23 &24.50 &5.34 &19.16 \\
692 EP &6170.30 &16.19 &0.02 &16.17 \\
694 LU &39477.28 &20.43 &0.07 &20.36 \\
696 BT &26169.55 &25.34 &6.62 &18.71 \\
698 SP &19620.09 &19.32 &3.66 &15.66 \\
700 FT &6094.07 &23.17 &0.36 &22.81 \\
709 \caption{The results of 90\%-10\% powers scenario}
712 \begin{tabular}{|*{6}{l|}}
714 Method & Energy & Energy & Performance & Distance \\
715 name & consumption/J & saving\% & degradation\% & \\
717 CG &2812.38 &36.36 &6.80 &29.56 \\
719 MG &825.427 &38.35 &6.41 &31.94 \\
721 EP &5281.62 &35.02 &2.68 &32.34 \\
723 LU &31611.28 &39.15 &3.51 &35.64 \\
725 BT &21296.46 &36.70 &6.60 &30.10 \\
727 SP &15183.42 &35.19 &11.76 &23.43 \\
729 FT &3856.54 &40.80 &5.67 &35.13 \\
738 \subfloat[Comparison the average of the results on 8 nodes]{%
739 \includegraphics[width=.22\textwidth]{fig/sen_comp}\label{fig:sen_comp}}%
741 \subfloat[Comparison the selected frequency scaling factors for 8 nodes]{%
742 \includegraphics[width=.24\textwidth]{fig/three_scenarios}\label{fig:scales_comp}}
744 \caption{The comparison of the three power scenarios}
747 To compare the results of these three powers scenarios, we are take the average of the performance degradation, the energy saving and the distances for all NAS benchmarks running on 8 or 9 nodes of class C, as in figure (\ref{fig:sen_comp}). Thus, according to the average of the results, the energy saving ratio is increased when using the a higher percentage for dynamic power (e.g. 90\%-10\% scenario). While the average of energy saving is decreased in 70\%-30\% scenario.
748 Because the static energy consumption is increase. Moreover, the average of distances is more related to energy saving changes. The average of the performance degradation is decreased when using a higher ratio for static power (e.g. 70\%-30\% scenario and 80\%-20\% scenario). The raison behind these relations, that the proposed algorithm optimize both energy consumption and performance in the same time. Therefore, when using a higher ratio for dynamic power the algorithm selecting bigger frequency scaling factors values, more energy saving versus more performance degradation, for example see the figure (\ref{fig:scales_comp}). The inverse happen when using a higher ratio for static power, the algorithm proportionally selects a smaller scaling values, less energy saving versus less performance degradation. This is because the
749 algorithm also keeps as much as possible the static energy consumption that is always related to execution time.
751 \subsection{The verifications of the proposed method}
753 The precision of the proposed algorithm mainly depends on the execution time prediction model and the energy model. The energy model is significantly depends on the execution time model EQ(\ref{eq:perf}), that the energy static related linearly. So, we are compare the predicted execution time with the real execution time (Simgrid time) values that gathered offline for the NAS benchmarks class B executed on 8 or 9 nodes. The execution time model can predicts
754 the real execution time by maximum normalized error 0.03 of all NAS benchmarks. The second verification that we are make is for the scaling algorithm to prove its ability to selects the best set of frequency scaling factors. Therefore, we are expand the algorithm to test at each iteration the frequency scaling factor of the slowest node with the all scaling factors available of the other nodes. This version of the algorithm is applied to different NAS benchmarks classes with different number of nodes. The results from the two algorithms is identical. While the proposed algorithm is runs faster, 10 times faster on average than the expanded algorithm.
760 \section*{Acknowledgment}
763 % trigger a \newpage just before the given reference
764 % number - used to balance the columns on the last page
765 % adjust value as needed - may need to be readjusted if
766 % the document is modified later
767 %\IEEEtriggeratref{15}
769 \bibliographystyle{IEEEtran}
770 \bibliography{IEEEabrv,my_reference}
777 %%% ispell-local-dictionary: "american"
780 % LocalWords: Fanfakh Charr FIXME Tianhe DVFS HPC NAS NPB SMPI Rauber's Rauber
781 % LocalWords: CMOS EQ EPSA Franche Comté Tflop Rünger IUT Maréchal Juin cedex
782 % LocalWords: de badri muslim MPI TcpOld TcmOld dNew dOld cp Sopt Tcp Tcm Ps
783 % LocalWords: Scp Fmax Fdiff SimGrid GFlops Xeon EP BT