\usepackage[T1]{fontenc}
\usepackage[utf8]{inputenc}
\usepackage[english]{babel}
-\usepackage{algorithm,algorithmicx,algpseudocode}
+\usepackage{algpseudocode}
\usepackage{graphicx,graphics}
\usepackage{subfig}
-\usepackage{listings}
-\usepackage{colortbl}
\usepackage{amsmath}
\usepackage{url}
\newcommand{\JC}[2][inline]{%
\todo[color=red!10,#1]{\sffamily\textbf{JC:} #2}\xspace}
+\newcommand{\Xsub}[2]{\ensuremath{#1_\textit{#2}}}
+
+\newcommand{\Dist}{\textit{Dist}}
+\newcommand{\Eind}{\Xsub{E}{ind}}
+\newcommand{\Enorm}{\Xsub{E}{Norm}}
+\newcommand{\Eoriginal}{\Xsub{E}{Original}}
+\newcommand{\Ereduced}{\Xsub{E}{Reduced}}
+\newcommand{\Fdiff}{\Xsub{F}{diff}}
+\newcommand{\Fmax}{\Xsub{F}{max}}
+\newcommand{\Fnew}{\Xsub{F}{new}}
+\newcommand{\Ileak}{\Xsub{I}{leak}}
+\newcommand{\Kdesign}{\Xsub{K}{design}}
+\newcommand{\MaxDist}{\textit{Max Dist}}
+\newcommand{\Ntrans}{\Xsub{N}{trans}}
+\newcommand{\Pdyn}{\Xsub{P}{dyn}}
+\newcommand{\PnormInv}{\Xsub{P}{NormInv}}
+\newcommand{\Pnorm}{\Xsub{P}{Norm}}
+\newcommand{\Tnorm}{\Xsub{T}{Norm}}
+\newcommand{\Pstates}{\Xsub{P}{states}}
+\newcommand{\Pstatic}{\Xsub{P}{static}}
+\newcommand{\Sopt}{\Xsub{S}{opt}}
+\newcommand{\Tcomp}{\Xsub{T}{comp}}
+\newcommand{\TmaxCommOld}{\Xsub{T}{Max Comm Old}}
+\newcommand{\TmaxCompOld}{\Xsub{T}{Max Comp Old}}
+\newcommand{\Tmax}{\Xsub{T}{max}}
+\newcommand{\Tnew}{\Xsub{T}{New}}
+\newcommand{\Told}{\Xsub{T}{Old}}
+
\begin{document}
\title{Dynamic Frequency Scaling for Energy Consumption
- Reduction in Distributed MPI Programs}
+ Reduction in Synchronous Distributed Applications}
\author{%
\IEEEauthorblockN{%
\begin{abstract}
Dynamic Voltage Frequency Scaling (DVFS) can be applied to modern CPUs. This
technique is usually used to reduce the energy consumed by a CPU while
- computing. Indeed, power consumption by a processor at a given time is
- exponentially related to its frequency. Thus, decreasing the frequency
+ computing. Thus, decreasing the frequency
reduces the power consumed by the CPU. However, it can also significantly
affect the performance of the executed program if it is compute bound and if a
- low CPU frequency is selected. The performance degradation ratio can even be
- higher than the saved energy ratio. Therefore, the chosen scaling factor must
+ low CPU frequency is selected. Therefore, the chosen scaling factor must
give the best possible trade-off between energy reduction and performance.
In this paper we present an algorithm that predicts the energy consumed with
consumption by the CPU and the performance of the application. The main
objective of HPC systems is to execute as fast as possible the application.
Therefore, our algorithm selects the scaling factor online with very small
-footprint. The proposed algorithm takes into account the communication times of
+overhead. The proposed algorithm takes into account the communication times of
the MPI program to choose the scaling factor. This algorithm has the ability to
predict both energy consumption and execution time over all available scaling
factors. The prediction achieved depends on some computing time information,
-gathered at the beginning of the runtime. We apply this algorithm to seven MPI
-benchmarks. These MPI programs are the NAS parallel benchmarks (NPB v3.3)
-developed by NASA~\cite{44}. Our experiments are executed using the simulator
-SimGrid/SMPI v3.10~\cite{Casanova:2008:SGF:1397760.1398183} over an homogeneous
+gathered at the beginning of the runtime. We apply this algorithm to the NAS parallel benchmarks (NPB v3.3)~\cite{44}. Our experiments are executed using the simulator
+SimGrid/SMPI v3.10~\cite{Casanova:2008:SGF:1397760.1398183} over a homogeneous
distributed memory architecture. Furthermore, we compare the proposed algorithm
with Rauber and Rünger methods~\cite{3}. The comparison's results show that our
algorithm gives better energy-time trade-off.
This paper is organized as follows: Section~\ref{sec.relwork} presents some
-related works from other authors. Section~\ref{sec.exe} explains the execution
-of parallel tasks and the sources of slack times. It also presents an energy
+related works from other authors. Section~\ref{sec.exe} presents an energy
model for homogeneous platforms. Section~\ref{sec.mpip} describes how the
performance of MPI programs can be predicted. Section~\ref{sec.compet} presents
the energy-performance objective function that maximizes the reduction of energy
gears and the execution time and the energy consumed with each frequency
gear are measured. Then a heuristic or an exact method uses the retrieved
information to compute the values of the scaling factor for the processors.
-In~\cite{29}, Xie et al. use an exact exponential breadth-first search algorithm
-to compute the scaling factor values that give the optimal energy reduction
-while respecting a deadline for a sequential program. They also present a
-linear heuristic that approximates the optimal solution. In~\cite{8} , Rountree
-et al. use a linear programming algorithm, while in~\cite{38,34}, Cochran et
+In~\cite{8} , Rountree et al. use a linear programming algorithm, while in~\cite{34}, Cochran et
al. use a multi-logistic regression algorithm for the same goal. The main
drawback of these methods is that they all require executing the
whole program or, a part of it, on all frequency gears for each new instance of the same program.
using a multimeter, the slack times, \dots{} Then a method will exploit these
measurements to compute the scaling factor values for each processor. This
operation, measurements and computing new scaling factor, can be repeated as
-much as needed if the iterations are not regular. Kimura, Peraza, Yu-Liang et
-al.~\cite{11,2,31} used varied heuristics to select the appropriate scaling
+much as needed if the iterations are not regular. Peraza, Yu-Liang et
+al.~\cite{2,31} used varied heuristics to select the appropriate scaling
factor values to eliminate the slack times during runtime. However, as seen
-in~\cite{39,19}, machine learning methods can take a lot of time to converge
+in~\cite{19}, machine learning method takes a lot of time to converge
when the number of available gears is big. To reduce the impact of slack times,
in~\cite{1}, Lim et al. developed an algorithm that detects the communication
sections and changes the frequency during these sections only. This approach
might change the frequency of each processor many times per iteration if an
iteration contains more than one communication section. In~\cite{3}, Rauber and
-Rünger used an analytical model that can predict the consumed energy and the
-execution time for every frequency gear after measuring the consumed energy and
-the execution time with the highest frequency gear. These predictions may be
-used to choose the optimal gear for each processor executing the parallel
-program to reduce energy consumption. To maintain the performance of the
-parallel program , they set the processor with the biggest load to the highest
-gear and then compute the scaling factor values for the rest of the processors.
-Although this model was built for parallel architectures, it can be adapted to
-distributed architectures by taking into account the communications. The
-primary contribution of our paper is to present a new online scaling factor
-selection method which has the following characteristics:
-\begin{enumerate}
-\item It is based on Rauber and Rünger analytical model to predict the energy
- consumption of the application with different frequency gears.
-\item It selects the frequency scaling factor for simultaneously optimizing
- energy reduction and maintaining performance.
-\item It is well adapted to distributed architectures because it takes into
- account the communication time.
-\item It is well adapted to distributed applications with imbalanced tasks.
-\item It has a very small footprint when compared to other methods
+Rünger used an analytical model that can predict the consumed energy for every frequency gear after measuring the consumed energy. They
+maintain the performance as mush as possible by setting the highest frequency gear to the slowest task.
+
+The primary contribution of
+our paper is to present a new online scaling factor selection method which has the
+ following characteristics:\\
+1) It is based on Rauber and Rünger analytical model to predict the energy
+ consumption of the application with different frequency gears.
+2) It selects the frequency scaling factor for simultaneously optimizing
+ energy reduction and maintaining performance.
+3) It is well adapted to distributed architectures because it takes into
+ account the communication time.
+4) It is well adapted to distributed applications with imbalanced tasks.
+5) It has a very small overhead when compared to other methods
(e.g.,~\cite{19}) and does not require profiling or training as
- in~\cite{38,34}.
-\end{enumerate}
-
+ in~\cite{34}.
-\section{Execution and energy of parallel tasks on homogeneous platform}
-\label{sec.exe}
% \JC{The whole subsection ``Parallel Tasks Execution on Homogeneous Platform'',
% can be deleted if we need space, we can just say we are interested in this
% paper in homogeneous clusters}
-\subsection{Parallel tasks execution on homogeneous platform}
-
-A homogeneous cluster consists in identical nodes in terms of hardware and
-software. Each node has its own memory and at least one processor which can be
-a multi-core. The nodes are connected via a high bandwidth network. Tasks
-executed on this model can be either synchronous or asynchronous. In this paper
-we consider execution of the synchronous tasks on distributed homogeneous
-platform. These tasks can exchange the data via synchronous message passing.
-\begin{figure*}[t]
- \centering
- \subfloat[Sync. imbalanced communications]{%
- \includegraphics[scale=0.67]{fig/commtasks}\label{fig:h1}}
- \subfloat[Sync. imbalanced computations]{%
- \includegraphics[scale=0.67]{fig/compt}\label{fig:h2}}
- \caption{Parallel tasks on homogeneous platform}
- \label{fig:homo}
-\end{figure*}
-Therefore, the execution time of a task consists in the computation time and the
-communication time. Moreover, the synchronous communications between tasks can
-lead to slack times while tasks wait at the synchronization barrier for other
-tasks to finish their tasks (see figure~(\ref{fig:h1})). The imbalanced
-communications happen when nodes have to send/receive different amounts of data
-or they communicate with different numbers of nodes. Other sources of slack
-times are imbalanced computations. This happens when processing different
-amounts of data on each processor (see figure~(\ref{fig:h2})). In this case the
-fastest tasks have to wait at the synchronization barrier for the slowest ones
-to begin the next task. In both cases the overall execution time of the program
-is the execution time of the slowest task as in EQ~(\ref{eq:T1}).
-\begin{equation}
- \label{eq:T1}
- \textit{Program Time} = \max_{i=1,2,\dots,N} T_i
-\end{equation}
-where $T_i$ is the execution time of task $i$ and all the tasks are executed
-concurrently on different processors.
-
-\subsection{Energy model for homogeneous platform}
+\section{Energy model for a homogeneous platform}
+\label{sec.exe}
Many researchers~\cite{9,3,15,26} divide the power consumed by a processor into
two power metrics: the static and the dynamic power. While the first one is
consumed as long as the computing unit is on, the latter is only consumed during
-computation times. The dynamic power $P_{dyn}$ is related to the switching
+computation times. The dynamic power $\Pdyn$ is related to the switching
activity $\alpha$, load capacitance $C_L$, the supply voltage $V$ and
-operational frequency $f$, as shown in EQ~(\ref{eq:pd}).
+operational frequency $f$, as shown in EQ~\eqref{eq:pd}.
\begin{equation}
\label{eq:pd}
- P_\textit{dyn} = \alpha \cdot C_L \cdot V^2 \cdot f
+ \Pdyn = \alpha \cdot C_L \cdot V^2 \cdot f
\end{equation}
-The static power $P_{static}$ captures the leakage power as follows:
+The static power $\Pstatic$ captures the leakage power as follows:
\begin{equation}
\label{eq:ps}
- P_\textit{static} = V \cdot N_{trans} \cdot K_{design} \cdot I_{leak}
+ \Pstatic = V \cdot \Ntrans \cdot \Kdesign \cdot \Ileak
\end{equation}
-where V is the supply voltage, $N_{trans}$ is the number of transistors,
-$K_{design}$ is a design dependent parameter and $I_{leak}$ is a
+where V is the supply voltage, $\Ntrans$ is the number of transistors,
+$\Kdesign$ is a design dependent parameter and $\Ileak$ is a
technology-dependent parameter. The energy consumed by an individual processor
to execute a given program can be computed as:
\begin{equation}
\label{eq:eind}
- E_\textit{ind} = P_\textit{dyn} \cdot T_{Comp} + P_\textit{static} \cdot T
+ \Eind = \Pdyn \cdot \Tcomp + \Pstatic \cdot T
\end{equation}
-where $T$ is the execution time of the program, $T_{Comp}$ is the computation
-time and $T_{Comp} \leq T$. $T_{Comp}$ may be equal to $T$ if there is no
+where $T$ is the execution time of the program, $\Tcomp$ is the computation
+time and $\Tcomp \leq T$. $\Tcomp$ may be equal to $T$ if there is no
communication, no slack time and no synchronization.
DVFS is a process that is allowed in modern processors to reduce the dynamic
constant $\beta$. This equation is used to study the change of the dynamic
voltage with respect to various frequency values in~\cite{3}. The reduction
process of the frequency can be expressed by the scaling factor $S$ which is the
-ratio between the maximum and the new frequency as in EQ~(\ref{eq:s}).
+ratio between the maximum and the new frequency as in EQ~\eqref{eq:s}.
\begin{equation}
\label{eq:s}
- S = \frac{F_\textit{max}}{F_\textit{new}}
+ S = \frac{\Fmax}{\Fnew}
\end{equation}
The value of the scaling factor $S$ is greater than 1 when changing the
frequency of the CPU to any new frequency value~(\emph{P-state}) in the
-governor. The CPU governor is an interface driver supplied by the operating
-system's kernel to lower a core's frequency. This factor reduces quadratically
+governor. This factor reduces quadratically
the dynamic power which may cause degradation in performance and thus, the
increase of the static energy because the execution time is increased~\cite{36}.
If the tasks are sorted according to their execution times before scaling in a
descending order, the total energy consumption model for a parallel homogeneous
platform, as presented by Rauber and Rünger~\cite{3}, can be written as a
-function of the scaling factor $S$, as in EQ~(\ref{eq:energy}).
+function of the scaling factor $S$, as in EQ~\eqref{eq:energy}.
\begin{equation}
\label{eq:energy}
- E = P_\textit{dyn} \cdot S_1^{-2} \cdot
+ E = \Pdyn \cdot S_1^{-2} \cdot
\left( T_1 + \sum_{i=2}^{N} \frac{T_i^3}{T_1^2} \right) +
- P_\textit{static} \cdot T_1 \cdot S_1 \cdot N
- \hfill
+ \Pstatic \cdot T_1 \cdot S_1 \cdot N
\end{equation}
-where $N$ is the number of parallel nodes, $T_i$ and $S_i$ for $i=1,\dots,N$ are
-the execution times and scaling factors of the sorted tasks. Therefore, $T1$ is
+where $N$ is the number of parallel nodes, $T_i$ for $i=1,\dots,N$ are
+the execution times of the sorted tasks. Therefore, $T_1$ is
the time of the slowest task, and $S_1$ its scaling factor which should be the
highest because they are proportional to the time values $T_i$. The scaling
-factors are computed as in EQ~(\ref{eq:si}).
+factors $S_i$ are computed as in EQ~\eqref{eq:si}.
\begin{equation}
\label{eq:si}
S_i = S \cdot \frac{T_1}{T_i}
- = \frac{F_\textit{max}}{F_\textit{new}} \cdot \frac{T_1}{T_i}
+ = \frac{\Fmax}{\Fnew} \cdot \frac{T_1}{T_i}
\end{equation}
-In this paper we use Rauber and Rünger's energy model, EQ~(\ref{eq:energy}), because it can be applied to homogeneous clusters if the communication time is taken in consideration. Moreover, we compare our algorithm with Rauber and Rünger's scaling factor selection
+In this paper we use Rauber and Rünger's energy model, EQ~\eqref{eq:energy}, because it can be applied to homogeneous clusters if the communication time is taken in consideration. Moreover, we compare our algorithm with Rauber and Rünger's scaling factor selection
method which uses the same energy model. In their method, the optimal scaling factor is
-computed by minimizing the derivation of EQ~(\ref{eq:energy}) which produces
-EQ~(\ref{eq:sopt}).
+computed by minimizing the derivation of EQ~\eqref{eq:energy} which produces
+EQ~\eqref{eq:sopt}.
\begin{equation}
\label{eq:sopt}
- S_\textit{opt} = \sqrt[3]{\frac{2}{N} \cdot \frac{P_\textit{dyn}}{P_\textit{static}} \cdot
+ \Sopt = \sqrt[3]{\frac{2}{N} \cdot \frac{\Pdyn}{\Pstatic} \cdot
\left( 1 + \sum_{i=2}^{N} \frac{T_i^3}{T_1^3} \right) }
\end{equation}
\section{Performance evaluation of MPI programs}
\label{sec.mpip}
-The performance (execution time) of parallel synchronous MPI applications depends
-on the time of the slowest task as in figure~(\ref{fig:homo}). If there is no
+The execution time of parallel synchronous MPI applications depends
+on the time of the slowest task. If there is no
communication and the application is not data bounded, the execution time of a
parallel program is linearly proportional to the operational frequency and any
DVFS operation for energy reduction increases the execution time of the parallel
be able to predict the execution time of MPI program, the communication time and
the computation time for the slowest task must be measured before scaling. These
times are used to predict the execution time for any MPI program as a function
-of the new scaling factor as in EQ~(\ref{eq:tnew}).
+of the new scaling factor as in EQ~\eqref{eq:tnew}.
\begin{equation}
\label{eq:tnew}
- \textit T_\textit{new} = T_\textit{Max Comp Old} \cdot S + T_{\textit{Max Comm Old}}
+ \Tnew = \TmaxCompOld \cdot S + \TmaxCommOld
\end{equation}
In this paper, this prediction method is used to select the best scaling factor
for each processor as presented in the next section.
This section presents our approach for choosing the optimal scaling factor.
This factor gives maximum energy reduction while taking into account the execution
-times for both computation and communication. The relation between the performance
-and the energy is nonlinear and complex. Thus, unlike the relation between the performance and the scaling factor, the relation of energy with the scaling factor is nonlinear, for more details refer to~\cite{17}. Moreover, they are not measured using the same metric. To
+times for both computation and communication. The relation between the execution time
+and the energy is nonlinear and complex. Thus, unlike the relation between the execution time and the scaling factor, the relation of energy with the scaling factor 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 energy by calculating the ratio between
the consumed energy with scaled frequency and the consumed energy without scaled
frequency:
\begin{multline}
\label{eq:enorm}
- E_\textit{Norm} = \frac{ E_\textit{Reduced}}{E_\textit{Original}} \\
- {} = \frac{P_\textit{dyn} \cdot S_1^{-2} \cdot
- \left( T_1 + \sum_{i=2}^{N}\frac{T_i^3}{T_1^2}\right) +
- P_\textit{static} \cdot T_1 \cdot S_1 \cdot N }{
- P_\textit{dyn} \cdot \left(T_1+\sum_{i=2}^{N}\frac{T_i^3}{T_1^2}\right) +
- P_\textit{static} \cdot T_1 \cdot N }
+ \Enorm = \frac{ \Ereduced}{\Eoriginal} \\
+ {} = \frac{\Pdyn \cdot S_1^{-2} \cdot
+ \left( T_1 + \sum_{i=2}^{N}\frac{T_i^3}{T_1^2}\right) +
+ \Pstatic \cdot T_1 \cdot S_1 \cdot N}{
+ \Pdyn \cdot \left(T_1+\sum_{i=2}^{N}\frac{T_i^3}{T_1^2}\right) +
+ \Pstatic \cdot T_1 \cdot N }
\end{multline}
-In the same way we can normalize the performance as follows:
+In the same way we can normalize the time as follows:
\begin{equation}
\label{eq:pnorm}
- P_\textit{Norm} = \frac{T_\textit{New}}{T_\textit{Old}}
- = \frac{T_\textit{Max Comp Old} \cdot S +
- T_\textit{Max Comm Old}}{T_\textit{Max Comp Old} +
- T_\textit{Max Comm Old}}
+ \Tnorm = \frac{\Tnew}{\Told}
+ = \frac{\TmaxCompOld \cdot S + \TmaxCommOld}{
+ \TmaxCompOld + \TmaxCommOld}
\end{equation}
The second problem is that the optimization operation for both energy and
-performance is not in the same direction. In other words, the normalized energy
-and the performance curves are not at the same direction see
-figure~(\ref{fig:r2}). While the main goal is to optimize the energy and
-performance in the same time. According to the equations~(\ref{eq:enorm})
-and~(\ref{eq:pnorm}), the scaling factor $S$ reduce both the energy and the
-performance simultaneously. But the main objective is to produce maximum energy
-reduction with minimum performance reduction. Many researchers used different
-strategies to solve this nonlinear problem for example see~\cite{19,42}, their
-methods add big overheads to the algorithm to select the suitable frequency.
-In this paper we present a method to find the optimal scaling factor $S$ to optimize both energy and performance simultaneously without adding a big
-overhead. Our solution for this problem is to make the optimization process
-for energy and performance follow the same direction. Therefore, we inverse the equation of the normalized
-performance as follows:
+execution time is not in the same direction. In other words, the normalized energy
+and the execution time curves are not at the same direction see
+Figure~\ref{fig:rel}\subref{fig:r2}. While the main goal is to optimize the
+energy and execution time in the same time. According to the
+equations~\eqref{eq:enorm} and~\eqref{eq:pnorm}, the scaling factor $S$ reduce
+both the energy and the execution time simultaneously. But the main objective is
+to produce maximum energy reduction with minimum execution time reduction. Many
+researchers used different strategies to solve this nonlinear problem for
+example see~\cite{19,42}, their methods add big overheads to the algorithm to
+select the suitable frequency. In this paper we present a method to find the
+optimal scaling factor $S$ to optimize both energy and execution time
+simultaneously without adding a big overhead. Our solution for this problem is
+to make the optimization process for energy and execution time follow the same
+direction. Therefore, we inverse the equation of the normalized execution time as
+follows:
\begin{equation}
\label{eq:pnorm_en}
- P^{-1}_\textit{Norm} = \frac{ T_\textit{Old}}{ T_\textit{New}}
- = \frac{T_\textit{Max Comp Old} +
- T_\textit{Max Comm Old}}{T_\textit{Max Comp Old} \cdot S +
- T_\textit{Max Comm Old}}
+ \Pnorm = \frac{ \Told}{ \Tnew}
+ = \frac{\TmaxCompOld +
+ \TmaxCommOld}{\TmaxCompOld \cdot S +
+ \TmaxCommOld}
\end{equation}
-\begin{figure*}
+\begin{figure}
\centering
- \subfloat[Converted relation.]{%
- \includegraphics[width=.4\textwidth]{fig/file}\label{fig:r1}}%
- \qquad%
\subfloat[Real relation.]{%
- \includegraphics[width=.4\textwidth]{fig/file3}\label{fig:r2}}
- \label{fig:rel}
+ \includegraphics[width=.5\linewidth]{fig/file3}\label{fig:r2}}%
+ \subfloat[Converted relation.]{%
+ \includegraphics[width=.5\linewidth]{fig/file}\label{fig:r1}}
\caption{The energy and performance relation}
-\end{figure*}
-Then, we can modelize our objective function as finding the maximum distance
-between the energy curve EQ~(\ref{eq:enorm}) and the inverse of performance
-curve EQ~(\ref{eq:pnorm_en}) over all available scaling factors. This
+ \label{fig:rel}
+\end{figure}
+Then, we can model our objective function as finding the maximum distance
+between the energy curve EQ~\eqref{eq:enorm} and the inverse of execution time (performance)
+curve EQ~\eqref{eq:pnorm_en} over all available scaling factors. This
represents the minimum energy consumption with minimum execution time (better
-performance) at the same time, see figure~(\ref{fig:r1}). Then our objective
-function has the following form:
+performance) at the same time, see Figure~\ref{fig:rel}\subref{fig:r1}. Then
+our objective function has the following form:
\begin{equation}
\label{eq:max}
- Max Dist = \max_{j=1,2,\dots,F}
- (\overbrace{P^{-1}_\textit{Norm}(S_j)}^{\text{Maximize}} -
- \overbrace{E_\textit{Norm}(S_j)}^{\text{Minimize}} )
+ \MaxDist = \max_{j=1,2,\dots,F}
+ (\overbrace{\Pnorm(S_j)}^{\text{Maximize}} -
+ \overbrace{\Enorm(S_j)}^{\text{Minimize}} )
\end{equation}
where $F$ is the number of available frequencies. Then we can select the optimal
-scaling factor that satisfies EQ~(\ref{eq:max}). Our objective function can
+scaling factor that satisfies EQ~\eqref{eq:max}. Our objective function can
work with any energy model or static power values stored in a data file.
Moreover, this function works in optimal way when the energy curve has a convex
form over the available frequency scaling factors as shown in~\cite{15,3,19}.
\section{Optimal scaling factor for performance and energy}
\label{sec.optim}
-Algorithm~\ref{EPSA} computes the optimal scaling factor according to the
-objective function described above.
-\begin{algorithm}[tp]
- \caption{Scaling factor selection algorithm}
- \label{EPSA}
+Algorithm on Figure~\ref{EPSA} computes the optimal scaling factor according to
+the objective function described above.
+\begin{figure}[tp]
\begin{algorithmic}[1]
- \State Initialize the variable $Dist=0$
- \State Set dynamic and static power values.
- \State Set $P_{states}$ to the number of available frequencies.
- \State Set the variable $F_{new}$ to max. frequency, $F_{new} = F_{max} $
- \State Set the variable $F_{diff}$ to the difference between two successive
- frequencies.
- \For {$j:=1$ to $P_{states} $}
- \State $F_{new}=F_{new} - F_{diff} $
- \State $S = \frac{F_\textit{max}}{F_\textit{new}}$
- \State $S_i = S \cdot \frac{T_1}{T_i}
- = \frac{F_\textit{max}}{F_\textit{new}} \cdot \frac{T_1}{T_i}$
+ % \footnotesize
+ \Require ~
+ \begin{description}
+ \item[$\Pstatic$] static power value
+ \item[$\Pdyn$] dynamic power value
+ \item[$\Pstates$] number of available frequencies
+ \item[$\Fmax$] maximum frequency
+ \item[$\Fdiff$] difference between two successive freq.
+ \end{description}
+ \Ensure $\Sopt$ is the optimal scaling factor
+
+ \State $\Sopt \gets 1$
+ \State $\Dist \gets 0$
+ \State $\Fnew \gets \Fmax$
+ \For {$j = 2$ to $\Pstates$}
+ \State $\Fnew \gets \Fnew - \Fdiff$
+ \State $S \gets \Fmax / \Fnew$
+ \State $S_i \gets S \cdot \frac{T_1}{T_i}
+ = \frac{\Fmax}{\Fnew} \cdot \frac{T_1}{T_i}$
for $i=1,\dots,N$
- \State $E_\textit{Norm} =
- \frac{P_\textit{dyn} \cdot S_1^{-2} \cdot
+ \State $\Enorm \gets
+ \frac{\Pdyn \cdot S_1^{-2} \cdot
\left( T_1 + \sum_{i=2}^{N}\frac{T_i^3}{T_1^2}\right) +
- P_\textit{static} \cdot T_1 \cdot S_1 \cdot N }{
- P_\textit{dyn} \cdot
+ \Pstatic \cdot T_1 \cdot S_1 \cdot N }{
+ \Pdyn \cdot
\left(T_1+\sum_{i=2}^{N}\frac{T_i^3}{T_1^2}\right) +
- P_\textit{static} \cdot T_1 \cdot N }$
- \State $P_{NormInv}=T_{old}/T_{new}$
- \If{$(P_{NormInv}-E_{Norm} > Dist)$}
- \State $S_{opt} = S$
- \State $Dist = P_{NormInv} - E_{Norm}$
+ \Pstatic \cdot T_1 \cdot N }$
+ \State $\Pnorm \gets \Told / \Tnew$
+ \If{$(\Pnorm - \Enorm > \Dist)$}
+ \State $\Sopt \gets S$
+ \State $\Dist \gets \Pnorm - \Enorm$
\EndIf
\EndFor
- \State Return $S_{opt}$
+ \State Return $\Sopt$
\end{algorithmic}
-\end{algorithm}
+ \caption{Scaling factor selection algorithm}
+ \label{EPSA}
+\end{figure}
The proposed algorithm works online during the execution time of the MPI
program. It selects the optimal scaling factor after gathering the computation
and communication times from the program after one iteration. Then the program
changes the new frequencies of the CPUs according to the computed scaling
-factors. This algorithm has a small execution time: for a homogeneous cluster
-composed of nodes having the characteristics presented in
-table~\ref{table:platform}, it takes \np[ms]{0.00152} on average for 4 nodes and
-\np[ms]{0.00665} on average for 32 nodes. The algorithm complexity is $O(F\cdot
-N)$, where $F$ is the number of available frequencies and $N$ is the number of
-computing nodes. The algorithm is called just once during the execution of the
-program. The DVFS algorithm~(\ref{dvfs}) shows where and when the algorithm is
-called in the MPI program.
-\begin{table}[htb]
- \caption{Platform file parameters}
- % title of Table
- \centering
- \begin{tabular}{|*{7}{l|}}
- \hline
- Max & Min & Backbone & Backbone & Link & Link & Sharing \\
- Freq. & Freq. & Bandwidth & Latency & Bandwidth & Latency & Policy \\
- \hline
- \np{2.5} & \np{800} & \np[GBps]{2.25} & \np[$\mu$s]{0.5} & \np[GBps]{1} & \np[$\mu$s]{50} & Full \\
- GHz & MHz & & & & & Duplex \\
- \hline
- \end{tabular}
- \label{table:platform}
-\end{table}
-
-\begin{algorithm}[tp]
- \caption{DVFS}
- \label{dvfs}
+factors. In our experiments over a homogeneous cluster described in
+Section~\ref{sec.expe}, this algorithm has a small execution time. It takes
+\np[$\mu$s]{1.52} on average for 4 nodes and \np[$\mu$s]{6.65} on average for 32
+nodes. The algorithm complexity is $O(F\cdot N)$, where $F$ is the number of
+available frequencies and $N$ is the number of computing nodes. The algorithm
+is called just once during the execution of the program. The DVFS algorithm on
+Figure~\ref{dvfs} shows where and when the algorithm is called in the MPI
+program.
+%\begin{table}[htb]
+% \caption{Platform file parameters}
+% % title of Table
+% \centering
+% \begin{tabular}{|*{7}{l|}}
+% \hline
+% Max & Min & Backbone & Backbone & Link & Link & Sharing \\
+% Freq. & Freq. & Bandwidth & Latency & Bandwidth & Latency & Policy \\
+% \hline
+% \np{2.5} & \np{800} & \np[GBps]{2.25} & \np[$\mu$s]{0.5} & \np[GBps]{1} & \np[$\mu$s]{50} & Full \\
+% GHz & MHz & & & & & Duplex \\
+% \hline
+% \end{tabular}
+% \label{table:platform}
+%\end{table}
+
+\begin{figure}[tp]
\begin{algorithmic}[1]
- \For {$k:=1$ to \textit{some iterations}}
+ % \footnotesize
+ \For {$k=1$ to \textit{some iterations}}
\State Computations section.
\State Communications section.
\If {$(k=1)$}
\State Gather all times of computation and\newline\hspace*{3em}%
communication from each node.
- \State Call algorithm~\ref{EPSA} with these times.
+ \State Call algorithm from Figure~\ref{EPSA} with these times.
\State Compute the new frequency from the\newline\hspace*{3em}%
- returned optimal scaling factor.
+ returned optimal scaling factor.
\State Set the new frequency to the CPU.
\EndIf
\EndFor
\end{algorithmic}
-\end{algorithm}
+ \caption{DVFS algorithm}
+ \label{dvfs}
+\end{figure}
After obtaining the optimal scaling factor, the program calculates the new
frequency $F_i$ for each task proportionally to its time value $T_i$. By
-substitution of EQ~(\ref{eq:s}) in EQ~(\ref{eq:si}), we can calculate the new
+substitution of EQ~\eqref{eq:s} in EQ~\eqref{eq:si}, we can calculate the new
frequency $F_i$ as follows:
\begin{equation}
\label{eq:fi}
- F_i = \frac{F_\textit{max} \cdot T_i}{S_\textit{optimal} \cdot T_\textit{max}}
+ F_i = \frac{\Fmax \cdot T_i}{\Sopt \cdot \Tmax}
\end{equation}
According to this equation all the nodes may have the same frequency value if
they have balanced workloads, otherwise, they take different frequencies when
-having imbalanced workloads. Thus, EQ~(\ref{eq:fi}) adapts the frequency of the
+having imbalanced workloads. Thus, EQ~\eqref{eq:fi} adapts the frequency of the
CPU to the nodes' workloads to maintain the performance of the program.
\section{Experimental results}
\label{sec.expe}
Our experiments are executed on the simulator SimGrid/SMPI v3.10. We configure
-the simulator to use a homogeneous cluster with one core per node. The detailed
-characteristics of our platform file are shown in
-table~(\ref{table:platform}). Each node in the cluster has 18 frequency values
+the simulator to use a homogeneous cluster with one core per node.
+%The detailed characteristics of our platform file are shown in Table~\ref{table:platform}.
+Each node in the cluster has 18 frequency values
from \np[GHz]{2.5} to \np[MHz]{800} with \np[MHz]{100} difference between each
-two successive frequencies. The simulated network link is \np[GB]{1} Ethernet
-(TCP/IP). The backbone of the cluster simulates a high performance switch.
+two successive frequencies. The nodes are connected via an ethernet network with 1Gbit/s bandwidth.
-\subsection{Performance prediction verification}
+\subsection{Execution time prediction verification}
-In this section we evaluate the precision of our performance prediction method
-based on EQ~(\ref{eq:tnew}) by applying it to the NAS benchmarks. The NAS programs
+In this section we evaluate the precision of our execution time prediction method
+based on EQ~\eqref{eq:tnew} by applying it to the NAS benchmarks. The NAS programs
are executed with the class B option to compare the real execution time with
the predicted execution time. Each program runs offline with all available
scaling factors on 8 or 9 nodes (depending on the benchmark) to produce real
execution time values. These scaling factors are computed by dividing the
-maximum frequency by the new one see EQ~(\ref{eq:s}).
-\begin{figure*}[t]
+maximum frequency by the new one see EQ~\eqref{eq:s}.
+\begin{figure}
\centering
- \includegraphics[width=.328\textwidth]{fig/cg_per}\hfill%
- \includegraphics[width=.328\textwidth]{fig/mg_pre}\hfill%
- % \includegraphics[width=.4\textwidth]{fig/bt_pre}\qquad%
- \includegraphics[width=.328\textwidth]{fig/lu_pre}\hfill%
- \caption{Comparing predicted to real execution time}
+ \includegraphics[width=.5\linewidth]{fig/cg_per}\hfill%
+ % \includegraphics[width=.5\linewidth]{fig/mg_pre}\hfill%
+ % \includegraphics[width=.5\linewidth]{fig/bt_pre}\qquad%
+ \includegraphics[width=.5\linewidth]{fig/lu_pre}\hfill%
+ \caption{Comparing predicted to real execution times}
\label{fig:pred}
-\end{figure*}
+\end{figure}
%see Figure~\ref{fig:pred}
In our cluster there are 18 available frequency states for each processor. This
leads to 18 run states for each program. We use seven MPI programs of the NAS
-parallel benchmarks: CG, MG, EP, FT, BT, LU and SP. Figure~(\ref{fig:pred})
-presents plots of the real execution times and the simulated ones. The maximum
+parallel benchmarks: CG, MG, EP, FT, BT, LU and SP. Figure~\ref{fig:pred}
+presents plots of the real execution times and the simulated ones. The maximum
normalized error between these two execution times varies between \np{0.0073} to
\np{0.031} dependent on the executed benchmark. The smallest prediction error
was for CG and the worst one was for LU.
\subsection{The experimental results for the scaling algorithm }
-
The proposed algorithm was applied to seven MPI programs of the NAS benchmarks
(EP, CG, MG, FT, BT, LU and SP) which were run with three classes (A, B and C).
For each instance the benchmarks were executed on a number of processors
proportional to the size of the class. Each class represents the problem size
-ascending from class A to C. Additionally, depending on some speed up
-points for each class we run the classes A, B and C on 4, 8 or 9 and 16 nodes
-respectively. Depending on EQ~(\ref{eq:energy}), we measure the energy
-consumption for all the NAS MPI programs while assuming that the dynamic power with
-the highest frequency is equal to \np[W]{20} and the power static is equal to
-\np[W]{4} for all experiments. These power values were also used by Rauber and
-Rünger in~\cite{3}. The results showed that the algorithm selected different
-scaling factors for each program depending on the communication features of the
-program as in the plots~(\ref{fig:nas}). These plots illustrate that there are
-different distances between the normalized energy and the normalized inverted
-performance curves, because there are different communication features for each
-benchmark. When there are little or no communications, the inverted
-performance curve is very close to the energy curve. Then the distance between
-the two curves is very small. This leads to small energy savings. The opposite
-happens when there are a lot of communication, the distance between the two
-curves is big. This leads to more energy savings (e.g. CG and FT), see
-table~(\ref{table:factors results}). All discovered frequency scaling factors
-optimize both the energy and the performance simultaneously for all NAS
-benchmarks. In table~(\ref{table:factors results}), we record all optimal
-scaling factors results for each benchmark running class C. These scaling
-factors give the maximum energy saving percentage and the minimum performance
-degradation percentage at the same time from all available scaling factors.
+ascending from class A to C. Additionally, depending on some speed up points
+for each class we run the classes A, B and C on 4, 8 or 9 and 16 nodes
+respectively. Depending on EQ~\eqref{eq:energy}, we measure the energy
+consumption for all the NAS MPI programs while assuming that the dynamic power
+with the highest frequency is equal to \np[W]{20} and the power static is equal
+to \np[W]{4} for all experiments. These power values were also used by Rauber
+and Rünger in~\cite{3}. The results showed that the algorithm selected
+different scaling factors for each program depending on the communication
+features of the program as in the plots from Figure~\ref{fig:nas}. These plots
+illustrate that there are different distances between the normalized energy and
+the normalized inverted execution time curves, because there are different
+communication features for each benchmark. When there are little or no
+communications, the inverted execution time curve is very close to the energy
+curve. Then the distance between the two curves is very small. This leads to
+small energy savings. The opposite happens when there are a lot of
+communication, the distance between the two curves is big. This leads to more
+energy savings (e.g. CG and FT), see Table~\ref{table:compareC}. All discovered
+frequency scaling factors optimize both the energy and the execution time
+simultaneously for all NAS benchmarks. In Table~\ref{table:compareC}, we record
+all optimal scaling factors results for each benchmark running class C. These
+scaling factors give the maximum energy saving percentage and the minimum
+performance degradation percentage at the same time from all available scaling
+factors.
\begin{figure*}[t]
\centering
- \includegraphics[width=.328\textwidth]{fig/ep}\hfill%
- \includegraphics[width=.328\textwidth]{fig/cg}\hfill%
- \includegraphics[width=.328\textwidth]{fig/sp}
- \includegraphics[width=.328\textwidth]{fig/lu}\hfill%
- \includegraphics[width=.328\textwidth]{fig/bt}\hfill%
- \includegraphics[width=.328\textwidth]{fig/ft}
+ \includegraphics[width=.33\linewidth]{fig/ep}\hfill%
+ \includegraphics[width=.33\linewidth]{fig/cg}\hfill%
+ % \includegraphics[width=.328\linewidth]{fig/sp}
+ % \includegraphics[width=.328\linewidth]{fig/lu}\hfill%
+ \includegraphics[width=.33\linewidth]{fig/bt}
+ % \includegraphics[width=.328\linewidth]{fig/ft}
\caption{Optimal scaling factors for the predicted energy and performance of NAS benchmarks}
\label{fig:nas}
\end{figure*}
-\begin{table}[htb]
- \caption{The scaling factors results}
- % title of Table
- \centering
- \begin{tabular}{|l|*{4}{r|}}
- \hline
- Program & Optimal & Energy & Performance & Energy-Perf. \\
- Name & Scaling Factor & Saving \% & Degradation \% & Distance \\
- \hline
- CG & 1.56 & 39.23 & 14.88 & 24.35 \\
- \hline
- MG & 1.47 & 34.97 & 21.70 & 13.27 \\
- \hline
- EP & 1.04 & 22.14 & 20.73 & 1.41 \\
- \hline
- LU & 1.38 & 35.83 & 22.49 & 13.34 \\
- \hline
- BT & 1.31 & 29.60 & 21.28 & 8.32 \\
- \hline
- SP & 1.38 & 33.48 & 21.36 & 12.12 \\
- \hline
- FT & 1.47 & 34.72 & 19.00 & 15.72 \\
- \hline
- \end{tabular}
- \label{table:factors results}
- % is used to refer this table in the text
-\end{table}
-As shown in table~(\ref{table:factors results}), when the optimal scaling
-factor has a big value we can gain more energy savings as in CG and
-FT benchmarks. The opposite happens when the optimal scaling factor has a small value as in BT and EP benchmarks. Our algorithm selects a big scaling factor value when the
+As shown in Table~\ref{table:compareC}, when the optimal scaling factor has a
+big value we can gain more energy savings as in CG and FT benchmarks. The
+opposite happens when the optimal scaling factor has a small value as in BT and
+EP benchmarks. Our algorithm selects a big scaling factor value when the
communication and the other slacks times are big and smaller ones in opposite
cases. In EP there are no communication inside the iterations. This leads our
algorithm to select smaller scaling factor values (inducing smaller energy
In this section, we compare our scaling factor selection method with Rauber and
Rünger methods~\cite{3}. They had two scenarios, the first is to reduce energy
-to the optimal level without considering the performance as in
-EQ~(\ref{eq:sopt}). We refer to this scenario as $R_{E}$. The second scenario
+to the optimal level without considering the execution time as in
+EQ~\eqref{eq:sopt}. We refer to this scenario as $R_{E}$. The second scenario
is similar to the first except setting the slower task to the maximum frequency
(when the scale $S=1$) to keep the performance from degradation as mush as
possible. We refer to this scenario as $R_{E-P}$. While we refer to our
algorithm as EPSA (Energy to Performance Scaling Algorithm). The comparison is
-made in tables \ref{table:compareA}, \ref{table:compareB},
-and~\ref{table:compareC}. These tables show the results of our method and
-Rauber and Rünger scenarios for all the NAS benchmarks programs for classes A, B
-and C.
-\begin{table}[p]
- \caption{Comparing results for the NAS class A}
- % title of Table
- \centering
- \begin{tabular}{|l|l|*{4}{r|}}
- \hline
- Method & Program & Factor & Energy & Performance & Energy-Perf. \\
- Name & Name & Value & Saving \% & Degradation \% & Distance \\
- \hline
- % \rowcolor[gray]{0.85}
- $EPSA$ & CG & 1.56 & 37.02 & 13.88 & 23.14 \\ \hline
- $R_{E-P}$ & CG & 2.14 & 42.77 & 25.27 & 17.50 \\ \hline
- $R_{E}$ & CG & 2.14 & 42.77 & 26.46 & 16.31 \\ \hline
-
- $EPSA$ & MG & 1.47 & 27.66 & 16.82 & 10.84 \\ \hline
- $R_{E-P}$ & MG & 2.14 & 34.45 & 31.84 & 2.61 \\ \hline
- $R_{E}$ & MG & 2.14 & 34.48 & 33.65 & 0.80 \\ \hline
-
- $EPSA$ & EP & 1.19 & 25.32 & 20.79 & 4.53 \\ \hline
- $R_{E-P}$ & EP & 2.05 & 41.45 & 55.67 & -14.22 \\ \hline
- $R_{E}$ & EP & 2.05 & 42.09 & 57.59 & -15.50 \\ \hline
-
- $EPSA$ & LU & 1.56 & 39.55 & 19.38 & 20.17 \\ \hline
- $R_{E-P}$ & LU & 2.14 & 45.62 & 27.00 & 18.62 \\ \hline
- $R_{E}$ & LU & 2.14 & 45.66 & 33.01 & 12.65 \\ \hline
-
- $EPSA$ & BT & 1.31 & 29.60 & 20.53 & 9.07 \\ \hline
- $R_{E-P}$ & BT & 2.10 & 45.53 & 49.63 & -4.10 \\ \hline
- $R_{E}$ & BT & 2.10 & 43.93 & 52.86 & -8.93 \\ \hline
-
- $EPSA$ & SP & 1.38 & 33.51 & 15.65 & 17.86 \\ \hline
- $R_{E-P}$ & SP & 2.11 & 45.62 & 42.52 & 3.10 \\ \hline
- $R_{E}$ & SP & 2.11 & 45.78 & 43.09 & 2.69 \\ \hline
-
- $EPSA$ & FT & 1.25 & 25.00 & 10.80 & 14.20 \\ \hline
- $R_{E-P}$ & FT & 2.10 & 39.29 & 34.30 & 4.99 \\ \hline
- $R_{E}$ & FT & 2.10 & 37.56 & 38.21 & -0.65 \\ \hline
- \end{tabular}
- \label{table:compareA}
- % is used to refer this table in the text
-\end{table}
-\begin{table}[p]
- \caption{Comparing results for the NAS class B}
- % title of Table
- \centering
- \begin{tabular}{|l|l|*{4}{r|}}
- \hline
- Method & Program & Factor & Energy & Performance & Energy-Perf. \\
- Name & Name & Value & Saving \% & Degradation \% & Distance \\
- \hline
- % \rowcolor[gray]{0.85}
- $EPSA$ & CG & 1.66 & 39.23 & 16.63 & 22.60 \\ \hline
- $R_{E-P}$ & CG & 2.15 & 45.34 & 27.60 & 17.74 \\ \hline
- $R_{E}$ & CG & 2.15 & 45.34 & 28.88 & 16.46 \\ \hline
-
- $EPSA$ & MG & 1.47 & 34.98 & 18.35 & 16.63 \\ \hline
- $R_{E-P}$ & MG & 2.14 & 43.55 & 36.42 & 7.13 \\ \hline
- $R_{E}$ & MG & 2.14 & 43.56 & 37.07 & 6.49 \\ \hline
+made in Table~\ref{table:compareC}. This table shows the results of our method and
+Rauber and Rünger scenarios for all the NAS benchmarks programs for class C.
- $EPSA$ & EP & 1.08 & 20.29 & 17.15 & 3.14 \\ \hline
- $R_{E-P}$ & EP & 2.00 & 42.38 & 56.88 & -14.50 \\ \hline
- $R_{E}$ & EP & 2.00 & 39.73 & 59.94 & -20.21 \\ \hline
-
- $EPSA$ & LU & 1.47 & 38.57 & 21.34 & 17.23 \\ \hline
- $R_{E-P}$ & LU & 2.10 & 43.62 & 36.51 & 7.11 \\ \hline
- $R_{E}$ & LU & 2.10 & 43.61 & 38.54 & 5.07 \\ \hline
-
- $EPSA$ & BT & 1.31 & 29.59 & 20.88 & 8.71 \\ \hline
- $R_{E-P}$ & BT & 2.10 & 44.53 & 53.05 & -8.52 \\ \hline
- $R_{E}$ & BT & 2.10 & 42.93 & 52.80 & -9.87 \\ \hline
-
- $EPSA$ & SP & 1.38 & 33.44 & 19.24 & 14.20 \\ \hline
- $R_{E-P}$ & SP & 2.15 & 45.69 & 43.20 & 2.49 \\ \hline
- $R_{E}$ & SP & 2.15 & 45.41 & 44.47 & 0.94 \\ \hline
-
- $EPSA$ & FT & 1.38 & 34.40 & 14.57 & 19.83 \\ \hline
- $R_{E-P}$ & FT & 2.13 & 42.98 & 37.35 & 5.63 \\ \hline
- $R_{E}$ & FT & 2.13 & 43.04 & 37.90 & 5.14 \\ \hline
- \end{tabular}
- \label{table:compareB}
- % is used to refer this table in the text
-\end{table}
-
-\begin{table}[p]
+\begin{table}
\caption{Comparing results for the NAS class C}
% title of Table
\centering
\begin{tabular}{|l|l|*{4}{r|}}
\hline
Method & Program & Factor & Energy & Performance & Energy-Perf. \\
- Name & Name & Value & Saving \% & Degradation \% & Distance \\
+ Name & Name & Value & Saving \% & Degradation \% & Distance \\
\hline
% \rowcolor[gray]{0.85}
$EPSA$ & CG & 1.56 & 39.23 & 14.88 & 24.35 \\ \hline
\label{table:compareC}
% is used to refer this table in the text
\end{table}
-As shown in tables~\ref{table:compareA},~\ref{table:compareB}
-and~\ref{table:compareC}, the ($R_{E-P}$) method outperforms the ($R_{E}$)
+As shown in Table~\ref{table:compareC}, the ($R_{E-P}$) method outperforms the ($R_{E}$)
method in terms of performance and energy reduction. The ($R_{E-P}$) method
also gives better energy savings than our method. However, although our scaling
-factor is not optimal for energy reduction, the results in these tables prove
+factor is not optimal for energy reduction, the results in this table prove
that our algorithm returns the best scaling factor that satisfy our objective
method: the largest distance between energy reduction and performance
-degradation. Figure~\ref{fig:compare} illustrates even better the distance between the energy reduction and performance degradation. The negative values mean that one of
+degradation. Figure~\ref{fig:compare} illustrates even better the distance between
+the energy reduction and performance degradation. The negative values mean that one of
the two objectives (energy or performance) have been degraded more than the
other. The positive trade-offs with the highest values lead to maximum energy
savings while keeping the performance degradation as low as possible. Our
algorithm always gives the highest positive energy to performance trade-offs
while Rauber and Rünger's method, ($R_{E-P}$), gives sometimes negative
trade-offs such as in BT and EP.
-\begin{figure*}[t]
+\begin{figure}[t]
\centering
- \includegraphics[width=.328\textwidth]{fig/compare_class_A}
- \includegraphics[width=.328\textwidth]{fig/compare_class_B}
- \includegraphics[width=.328\textwidth]{fig/compare_class_C}
+% \includegraphics[width=.328\linewidth]{fig/compare_class_A}
+% \includegraphics[width=.328\linewidth]{fig/compare_class_B}
+ \includegraphics[width=\linewidth]{fig/compare_class_C}
\caption{Comparing our method to Rauber and Rünger's methods}
\label{fig:compare}
-\end{figure*}
+\end{figure}
\section{Conclusion}
\label{sec.concl}
In this paper, we have presented a new online scaling factor selection method
that optimizes simultaneously the energy and performance of a distributed
-application running on an homogeneous cluster. It uses the computation and
+application running on a homogeneous cluster. It uses the computation and
communication times measured at the first iteration to predict energy
-consumption and the performance of the parallel application at every available
+consumption and the execution time of the parallel application at every available
frequency. Then, it selects the scaling factor that gives the best trade-off
between energy reduction and performance which is the maximum distance between
-the energy and the inverted performance curves. To evaluate this method, we
+the energy and the inverted eexecution time curves. To evaluate this method, we
have applied it to the NAS benchmarks and it was compared to Rauber and Rünger
methods while being executed on the simulator SimGrid. The results showed that
our method, outperforms Rauber and Rünger's methods in terms of energy-performance
-ratio.
+ratio.
In the near future, we would like to adapt this scaling factor selection method
to heterogeneous platforms where each node has different characteristics. In
