Corrections + reindent source code.

[mpi-energy.git] / paper.tex

diff --git a/paper.tex b/paper.tex
index 1ce2f6034c87f4cf2da2a87007c3943215805bc8..8039f59d1c098b1df5081f3ee0ec978ce698df2d 100644 (file)
--- a/paper.tex
+++ b/paper.tex
@@ -9,11 +9,10 @@
 \usepackage{listings}
 \usepackage{colortbl}
 \usepackage{amsmath}
 \usepackage{listings}
 \usepackage{colortbl}
 \usepackage{amsmath}

-% \usepackage{sectsty}
-% \usepackage{titlesec}
-% \usepackage{secdot}
-%\usepackage[font={footnotesize,bt}]{caption}
-%\usepackage[font=scriptsize,labelfont=bf]{caption}
+
+\usepackage[autolanguage,np]{numprint}
+\renewcommand*\npunitcommand[1]{\text{#1}}
+

 \usepackage{xspace}
 \usepackage[textsize=footnotesize]{todonotes}
 \newcommand{\AG}[2][inline]{\todo[color=green!50,#1]{\sffamily\textbf{AG:} #2}\xspace}
 \usepackage{xspace}
 \usepackage[textsize=footnotesize]{todonotes}
 \newcommand{\AG}[2][inline]{\todo[color=green!50,#1]{\sffamily\textbf{AG:} #2}\xspace}


@@ -24,9 +23,9 @@
 
 \author{%
   \IEEEauthorblockN{%
 
 \author{%
   \IEEEauthorblockN{%

-    Ahmed Badri,

     Jean-Claude Charr,
     Jean-Claude Charr,

-    Raphaël Couturier and
+    Raphaël Couturier,
+    Ahmed Fanfakh and

     Arnaud Giersch
   }
   \IEEEauthorblockA{%
     Arnaud Giersch
   }
   \IEEEauthorblockA{%


@@ -41,7 +40,18 @@
   Complete affiliation, add an email address, etc.}
 
 \begin{abstract}
   Complete affiliation, add an email address, etc.}
 
 \begin{abstract}

-  \AG{complete the abstract\dots}
+  The important technique for energy reduction of parallel systems is CPU
+  frequency scaling. This operation is used by many researchers to reduce energy
+  consumption in many ways. Frequency scaling operation also has a big impact on
+  the performances. In some cases, the performance degradation ratio is bigger
+  than energy saving ratio when the frequency is scaled to low level. Therefore,
+  the trade offs between the energy and performance becomes more important topic
+  when using this technique. In this paper we developed an algorithm that select
+  the frequency scaling factor for both energy and performance simultaneously.
+  This algorithm takes into account the communication times when selecting the
+  frequency scaling factor. It works online without training or profiling to
+  have a very small overhead.  The algorithm has better energy-performance trade
+  offs compared to other methods.

 \end{abstract}
 
 \section{Introduction}
 \end{abstract}
 
 \section{Introduction}


@@ -72,12 +82,12 @@ of the performance. It is important to notice that lowering the frequency to
 minimum value does not always give the most efficient execution due to energy
 leakage. The best scaling factor might be chosen during execution (online) or
 during a pre-execution phase.  In this paper we emphasize to develop an
 minimum value does not always give the most efficient execution due to energy
 leakage. The best scaling factor might be chosen during execution (online) or
 during a pre-execution phase.  In this paper we emphasize to develop an

-algorithm that selects the optimal frequency scaling factor that takes into
-consideration simultaneously the energy consumption and the performance. The
+algorithm that selects a frequency scaling factor that simultaneously takes into
+consideration  the energy consumption and the performance. The

 main objective of HPC systems is to run the application with less execution
 main objective of HPC systems is to run the application with less execution

-time. Therefore, our algorithm selects the optimal scaling factor online with
+time. Therefore, our algorithm selects the scaling factor online with

 very small footprint. The proposed algorithm takes into account the
 very small footprint. The proposed algorithm takes into account the

-communication times of the MPI programs to choose the scaling factor. This
+communication times of the MPI program to choose the scaling factor. This

 algorithm has 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
 algorithm has 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


@@ -85,16 +95,20 @@ 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 distributed memory architecture. Furthermore, we compare the
 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 distributed memory architecture. Furthermore, we compare the

-proposed algorithm with Rauber's methods.
-\AG{Add citation for Rauber's methods.  Moreover, Rauber was not alone to to this work (use ``Rauber et al.'', or ``Rauber and Gudula'', or \dots)}
+proposed algorithm with Rauber and Rünger methods~\cite{3}.

 The comparison's results show that our
 algorithm gives better energy-time trade off.
 The comparison's results show that our
 algorithm gives better energy-time trade off.

-%
-\AG{Correctly reword the following}%
-In Section~\ref{sec.relwork} we present works from other
-authors. Then, in Sections~\ref{sec.ptasks} and~\ref{sec.energy}, we
-introduce our model. [\dots] Finally, we conclude in
-Section~\ref{sec.concl}.
+
+This paper is organized as follows: Section~\ref{sec.relwork} presents the works
+from other authors.  Section~\ref{sec.ptasks} shows the execution of parallel
+tasks and sources of idle times. Section~\ref{sec.energy} resumes the energy
+model of homogeneous platform. Section~\ref{sec.mpip} evaluates the performance
+of MPI program.  Section~\ref{sec.verif} verifies the performance prediction
+model. Section~\ref{sec.compet} presents the energy-performance trade offs
+objective function. Section~\ref{sec.optim} demonstrates the proposed
+energy-performance algorithm. Section~\ref{sec.expe} presents the results of our
+experiments.  Section~\ref{sec.compare} shows the comparison results. Finally,
+we conclude in Section~\ref{sec.concl}.

 
 \section{Related Works}
 \label{sec.relwork}
 
 \section{Related Works}
 \label{sec.relwork}


@@ -102,56 +116,54 @@ Section~\ref{sec.concl}.
 \AG{Consider introducing the models (sec.~\ref{sec.ptasks},
   maybe~\ref{sec.energy}) before related works}
 
 \AG{Consider introducing the models (sec.~\ref{sec.ptasks},
   maybe~\ref{sec.energy}) before related works}
 

-In the this section some heuristics, to compute the scaling factor, are
-presented and classified in two parts : offline and online methods.
+In the this section some heuristics to compute the scaling factor are
+presented and classified in two parts: offline and online methods.

 
 \subsection{The offline DVFS orientations}
 
 The DVFS offline methods are static and are not executed during the runtime of
 the program. Some approaches used heuristics to select the best DVFS state
 
 \subsection{The offline DVFS orientations}
 
 The DVFS offline methods are static and are not executed during the runtime of
 the program. Some approaches used heuristics to select the best DVFS state

-during the compilation phases as an example in Azevedo et al.~\cite{40}. He used
-intra-task algorithm
-\AG{what is an ``intra-task algorithm''?}
-to choose the DVFS setting when there are dependency points
-between tasks. While in~\cite{29}, Xie et al. used breadth-first search
-algorithm to do that. Their goal is saving energy with time limits. Another
-approaches gathers and stores the runtime information for each DVFS state, then
-used their methods offline to select the suitable DVFS that optimize energy-time
-trade offs. As an example~\cite{8}, Rountree et al. used liner programming
-algorithm, while in~\cite{38,34}, Cochran et al. used multi logistic regression
-algorithm for the same goal. The offline study that shown the DVFS impact on the
-communication time of the MPI program is~\cite{17}, Freeh et al. show that these
-times not changed when the frequency is scaled down.
+during the compilation phases as for example in Azevedo et al.~\cite{40}. They
+use dynamic voltage scaling (DVS) algorithm to choose the DVS setting when there
+are dependency points between tasks. While in~\cite{29}, Xie et al. used
+breadth-first search algorithm to do that. Their goal is to save energy with
+time limits. Another approach gathers and stores the runtime information for
+each DVFS state, then selects the suitable DVFS offline to optimize energy-time
+trade offs. As an example, Rountree et al.~\cite{8} use liner programming
+algorithm, while in~\cite{38,34}, Cochran et al. use multi logistic regression
+algorithm for the same goal. The offline study that shows the DVFS impact on the
+communication time of the MPI program is~\cite{17}, where Freeh et al. show that
+these times do not change when the frequency is scaled down.

 
 \subsection{The online DVFS orientations}
 
 
 \subsection{The online DVFS orientations}
 

-The objective of these works is to dynamically compute and set the frequency of
-the CPU during the runtime of the program for saving energy. Estimating and
-predicting approaches for the energy-time trade offs developed by
-~\cite{11,2,31}. These works select the best DVFS setting depending on the slack
-times. These times happen when the processors have to wait for data from other
-processors to compute their task. For example, during the synchronous
-communication time that take place in the MPI programs, the processors are
-idle. The optimal DVFS can be selected using the learning methods. Therefore, in
-~\cite{39,19} used machine learning to converge to the suitable DVFS
-configuration. Their learning algorithms have big time to converge when the
-number of available frequencies is high. Also, the communication time of the MPI
-program used online for saving energy as in~\cite{1}, Lim et al. developed an
-algorithm that detects the communication sections and changes the frequency
-during these sections only. This approach changes the frequency many times
-because an iteration may contain more than one communication section. The domain
-of analytical modeling used for choosing the optimal frequency as in~\cite{3},
-Rauber et al. developed an analytical mathematical model for determining the
-optimal frequency scaling factor for any number of concurrent tasks, without
-considering communication times. They set the slowest task to maximum frequency
-for maintaining performance.  In this paper we compare our algorithm with
-Rauber's model~\cite{3}, because his model can be used for any number of
-concurrent tasks for homogeneous platform and this is the same direction of this
-paper.  However, the primary contributions of this paper are:
+The objective of the online DVFS orientations is to dynamically compute and set
+the frequency of the CPU for saving energy during the runtime of the
+programs. Estimating and predicting approaches for the energy-time trade offs
+are developed by Kimura, Peraza, Yu-Liang et al.  ~\cite{11,2,31}. These works
+select the best DVFS setting depending on the slack times. These times happen
+when the processors have to wait for data from other processors to compute their
+task. For example, during the synchronous communications that take place in MPI
+programs, some processors are idle. The optimal DVFS can be selected using
+learning methods. Therefore, in Dhiman, Hao Shen et al.  ~\cite{39,19} used
+machine learning to converge to the suitable DVFS configuration. Their learning
+algorithms take big time to converge when the number of available frequencies is
+high. Also, the communication sections of the MPI program can be used to save
+energy. In~\cite{1}, Lim et al. developed an algorithm that detects the
+communication sections and changes the frequency during these sections
+only. This approach changes the frequency many times because an iteration may
+contain more than one communication section. The domain of analytical modeling
+can also be used for choosing the optimal frequency as in Rauber and
+Rünger~\cite{3}. They developed an analytical mathematical model to determine
+the optimal frequency scaling factor for any number of concurrent tasks. They
+set the slowest task to maximum frequency for maintaining performance.  In this
+paper we compare our algorithm with Rauber and Rünger model~\cite{3}, because
+their model can be used for any number of concurrent tasks for homogeneous
+platforms. The primary contributions of this paper are:

 \begin{enumerate}
 \begin{enumerate}

-\item Selecting the optimal frequency scaling factor for energy and performance
-  simultaneously. While taking into account the communication time.
-\item Adapting our scale factor to taking into account the imbalanced tasks.
+\item Selecting the frequency scaling factor for simultaneously optimizing energy and performance,
+   while taking into account the communication time.
+\item Adapting our scaling factor to take into account the imbalanced tasks.

 \item The execution time of our algorithm is very small when compared to other
   methods (e.g.,~\cite{19}).
 \item The proposed algorithm works online without profiling or training as
 \item The execution time of our algorithm is very small when compared to other
   methods (e.g.,~\cite{19}).
 \item The proposed algorithm works online without profiling or training as


@@ -161,64 +173,61 @@ paper.  However, the primary contributions of this paper are:
 \section{Parallel Tasks Execution on Homogeneous Platform}
 \label{sec.ptasks}
 
 \section{Parallel Tasks Execution on Homogeneous Platform}
 \label{sec.ptasks}
 

-A homogeneous cluster consists of identical nodes in terms of the hardware and
-the software. Each node has its own memory and at least one processor which can
+A homogeneous cluster consists of 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
 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 memory passing.
+platform. These tasks can exchange the data via synchronous message passing.

 \begin{figure*}[t]
   \centering
 \begin{figure*}[t]
   \centering

-  \subfloat[Sync. Imbalanced Communications]{\includegraphics[scale=0.67]{synch_tasks}\label{fig:h1}}
+  \subfloat[Sync. Imbalanced Communications]{\includegraphics[scale=0.67]{commtasks}\label{fig:h1}}

   \subfloat[Sync. Imbalanced Computations]{\includegraphics[scale=0.67]{compt}\label{fig:h2}}
   \caption{Parallel Tasks on Homogeneous Platform}
   \label{fig:homo}
 \end{figure*}
   \subfloat[Sync. Imbalanced Computations]{\includegraphics[scale=0.67]{compt}\label{fig:h2}}
   \caption{Parallel Tasks on Homogeneous Platform}
   \label{fig:homo}
 \end{figure*}

-\AG{On fig.~\ref{fig:h1}, how can there be a synchronization point without communications just before ?\\
-Use ``Sync.'' to abbreviate ``Synchronization''}

 Therefore, the execution time of a task consists of the computation time and the
 communication time. Moreover, the synchronous communications between tasks can
 Therefore, the execution time of a task consists of the computation time and the
 communication time. Moreover, the synchronous communications between tasks can

-lead to idle time while tasks wait at the synchronous point for others tasks to
-finish their communications see figure~(\ref{fig:h1}).  Another source for idle
-times is the imbalanced computations. This happen when processing different
-amounts of data on each processor as an example see figure~(\ref{fig:h2}). In
-this case the fastest tasks have to wait at the synchronous barrier for the
-slowest tasks to finish their job. In both two cases the overall execution time
-of the program is the execution time of the slowest task as :
+lead to idle time while tasks wait at the synchronization barrier for other tasks to
+finish their communications (see figure~(\ref{fig:h1})). The imbalanced communications happen when nodes have to send/receive different amount of data or each node is communicates with different number of nodes. Another source for idle times is the imbalanced computations. This happen 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 tasks to finish their job. In both cases the overall execution time
+of the program is the execution time of the slowest task as:

 \begin{equation}
   \label{eq:T1}
   \textit{Program Time} = \max_{i=1,2,\dots,N} T_i
 \end{equation}
 \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 process $i$.
+where $T_i$ is the execution time of task $i$.

 
 \section{Energy Model for Homogeneous Platform}
 \label{sec.energy}
 
 
 \section{Energy Model for Homogeneous Platform}
 \label{sec.energy}
 

-The energy consumption by the processor consists of two powers metric: the
+The energy consumption by the processor consists of two power metrics: the

 dynamic and the static power. This general power formulation is used by many
 dynamic and the static power. This general power formulation is used by many

-researchers see~\cite{9,3,15,26}. The dynamic power of the CMOS processors
+researchers~\cite{9,3,15,26}. The dynamic power of the CMOS processors

 $P_{dyn}$ is related to the switching activity $\alpha$, load capacitance $C_L$,
 $P_{dyn}$ is related to the switching activity $\alpha$, load capacitance $C_L$,

-the supply voltage $V$ and operational frequency $f$ respectively as follow :
+the supply voltage $V$ and operational frequency $f$ respectively as follow:

 \begin{equation}
   \label{eq:pd}
 \begin{equation}
   \label{eq:pd}

-  P_{dyn} = \alpha \cdot C_L \cdot V^2 \cdot f
+  P_\textit{dyn} = \alpha \cdot C_L \cdot V^2 \cdot f

 \end{equation}
 The static power $P_{static}$ captures the leakage power consumption as well as
 the power consumption of peripheral devices like the I/O subsystem.
 \begin{equation}
   \label{eq:ps}
 \end{equation}
 The static power $P_{static}$ captures the leakage power consumption as well as
 the power consumption of peripheral devices like the I/O subsystem.
 \begin{equation}
   \label{eq:ps}

-  P_{static}  = V \cdot N \cdot K_{design} \cdot I_{leak}
+   P_\textit{static}  = V \cdot N \cdot K_{design} \cdot I_{leak}

 \end{equation}
 where V is the supply voltage, N is the number of transistors, $K_{design}$ is a
 design dependent parameter and $I_{leak}$ is a technology-dependent
 parameter. Energy consumed by an individual processor $E_{ind}$ is the summation
 \end{equation}
 where V is the supply voltage, N is the number of transistors, $K_{design}$ is a
 design dependent parameter and $I_{leak}$ is a technology-dependent
 parameter. Energy consumed by an individual processor $E_{ind}$ is the summation

-of the dynamic and the static power multiply by the execution time for example
+of the dynamic and the static power multiplied by the execution time for example

 see~\cite{36,15}.
 \begin{equation}
   \label{eq:eind}
 see~\cite{36,15}.
 \begin{equation}
   \label{eq:eind}

-  E_{ind} = ( P_{dyn} + P_{static} ) \cdot T
+   E_\textit{ind} = ( P_\textit{dyn} + P_\textit{static} ) \cdot T

 \end{equation}
 \end{equation}

-The dynamic voltage and frequency scaling (DVFS) is a process that allowed in
+The dynamic voltage and frequency scaling (DVFS) is a process that is allowed in

 modern processors to reduce the dynamic power by scaling down the voltage and
 frequency. Its main objective is to reduce the overall energy
 consumption~\cite{37}. The operational frequency \emph f depends linearly on the
 modern processors to reduce the dynamic power by scaling down the voltage and
 frequency. Its main objective is to reduce the overall energy
 consumption~\cite{37}. The operational frequency \emph f depends linearly on the


@@ -229,29 +238,29 @@ expressed by scaling factor \emph S. The scale \emph S is the ratio between the
 maximum and the new frequency as in EQ~(\ref{eq:s}).
 \begin{equation}
   \label{eq:s}
 maximum and the new frequency as in EQ~(\ref{eq:s}).
 \begin{equation}
   \label{eq:s}

-  S = \frac{F_{max}}{F_{new}}
+ S = \frac{F_\textit{max}}{F_\textit{new}}

 \end{equation}
 \end{equation}

-The value of the scale $S$ is greater than 1 when changing the frequency to
-any new frequency value (\emph {P-state}) in governor.
-\AG{Explain what's a governor}
-It is equal to 1 when the
-frequency are set to the maximum frequency.  The energy consumption model for
-parallel homogeneous platform is depending on the scaling factor \emph S. This
-factor reduces quadratically the dynamic power.  Also, this factor increases the
-static energy linearly because the execution time is increased~\cite{36}.  The
-energy model, depending on the frequency scaling factor, of homogeneous platform
-for any number of concurrent tasks develops by Rauber~\cite{3}. This model
-consider the two powers metric for measuring the energy of the parallel tasks as
-in EQ~(\ref{eq:energy}).
+The value of the scale $S$ is greater than 1 when changing the frequency to any
+new frequency value~(\emph {P-state}) in governor, the CPU governor is an
+interface driver supplied by the operating system kernel (e.g. Linux) to
+lowering core's frequency.  The scaling factor is equal to 1 when the frequency
+set is to the maximum frequency.  The energy consumption model for parallel
+homogeneous platform depends on the scaling factor \emph S. This factor reduces
+quadratically the dynamic power.  Also, this factor increases the static energy
+linearly because the execution time is increased~\cite{36}.  The energy model
+depending on the frequency scaling factor for homogeneous platform for any
+number of concurrent tasks was developed by Rauber and Rünger~\cite{3}. This
+model considers the two power metrics for measuring the energy of the parallel
+tasks as in EQ~(\ref{eq:energy}):

 
 \begin{equation}
   \label{eq:energy}
 
 \begin{equation}
   \label{eq:energy}

-  E = P_{dyn} \cdot S_1^{-2} \cdot
+  E = P_\textit{dyn} \cdot S_1^{-2} \cdot

     \left( T_1 + \sum_{i=2}^{N} \frac{T_i^3}{T_1^2} \right) +
     \left( T_1 + \sum_{i=2}^{N} \frac{T_i^3}{T_1^2} \right) +

-    P_{static} \cdot T_1 \cdot S_1 \cdot N
+    P_\textit{static} \cdot T_1 \cdot S_1 \cdot N

  \hfill
 \end{equation}
  \hfill
 \end{equation}

-Where \emph N is the number of parallel nodes, $T_1 $ is the time of the slower
+where \emph N is the number of parallel nodes, $T_1 $ is the time of the slowest

 task, $T_i$ is the time of the task $i$ and $S_1$ is the maximum scaling factor
 for the slower task. The scaling factor $S_1$, as in EQ~(\ref{eq:s1}), selects
 from the set of scales values $S_i$. Each of these scales are proportional to
 task, $T_i$ is the time of the task $i$ and $S_1$ is the maximum scaling factor
 for the slower task. The scaling factor $S_1$, as in EQ~(\ref{eq:s1}), selects
 from the set of scales values $S_i$. Each of these scales are proportional to


@@ -263,51 +272,51 @@ the time value $T_i$ depends on the new frequency value as in EQ~(\ref{eq:si}).
 \begin{equation}
   \label{eq:si}
   S_i = S \cdot \frac{T_1}{T_i}
 \begin{equation}
   \label{eq:si}
   S_i = S \cdot \frac{T_1}{T_i}

-      = \frac{F_{max}}{F_{new}} \cdot \frac{T_1}{T_i}
+      = \frac{F_\textit{max}}{F_\textit{new}} \cdot \frac{T_1}{T_i}

 \end{equation}
 \end{equation}

-Where $F$ is the number of available frequencies. In this paper we depend on
-Rauber's energy model EQ~(\ref{eq:energy}) for two reasons : 1-this model used
-for homogeneous platform that we work on in this paper. 2-we are compare our
-algorithm with Rauber's scaling model.  Rauber's optimal scaling factor for
-optimal energy reduction derived from the EQ~(\ref{eq:energy}). He takes the
-derivation for this equation (to be minimized) and set it to zero to produce the
-scaling factor as in EQ~(\ref{eq:sopt}).
+where $F$ is the number of available frequencies. In this paper we depend on
+Rauber and Rünger energy model EQ~(\ref{eq:energy}) for two reasons: (1) this
+model is used for homogeneous platform that we work on in this paper, and (2) we
+compare our algorithm with Rauber and Rünger scaling model.  Rauber and Rünger
+scaling factor that reduce energy consumption derived from the
+EQ~(\ref{eq:energy}). They take the derivation for this equation (to be
+minimized) and set it to zero to produce the scaling factor as in
+EQ~(\ref{eq:sopt}).

 \begin{equation}
   \label{eq:sopt}
 \begin{equation}
   \label{eq:sopt}

-  S_{opt} = \sqrt[3]{\frac{2}{n} \cdot \frac{P_{dyn}}{P_{static}} \cdot
+  S_\textit{opt} = \sqrt[3]{\frac{2}{n} \cdot \frac{P_\textit{dyn}}{P_\textit{static}} \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}
 
     \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 the parallel MPI applications are depends on
+The performance (execution time) of  parallel MPI applications depend on

 the time of the slowest task as in figure~(\ref{fig:homo}). Normally the
 execution time of the parallel programs are proportional to the operational
 the time of the slowest task as in figure~(\ref{fig:homo}). Normally the
 execution time of the parallel programs are proportional to the operational

-frequency. Therefore, any DVFS operation for the energy reduction increase the
+frequency. Therefore, any DVFS operation for the energy reduction increases the

 execution time of the parallel program. As shown in EQ~(\ref{eq:energy}) the
 execution time of the parallel program. As shown in EQ~(\ref{eq:energy}) the

-energy affected by the scaling factor $S$. This factor also has a great impact
+energy is affected by the scaling factor $S$. This factor also has a great impact

 on the performance. When scaling down the frequency to the new value according
 on the performance. When scaling down the frequency to the new value according

-to EQ~(\ref{eq:s}) lead to the value of the scale $S$ has inverse relation with
-new frequency value ($S \propto \frac{1}{F_{new}}$). Also when decrease the
-frequency value, the execution time increase. Then the new frequency value has
-inverse relation with time ($F_{new} \propto \frac{1}{T}$). This lead to the
+to EQ~(\ref{eq:s}), the value of the scale $S$ has inverse relation with
+new frequency value ($S \propto \frac{1}{F_{new}}$). Also when decreasing the
+frequency value, the execution time increases. Then the new frequency value has
+inverse relation with time ($F_{new} \propto \frac{1}{T}$). This leads to the

 frequency scaling factor $S$ proportional linearly with execution time ($S
 \propto T$). Large scale MPI applications such as NAS benchmarks have
 considerable amount of communications embedded in these programs. During the
 frequency scaling factor $S$ proportional linearly with execution time ($S
 \propto T$). Large scale MPI applications such as NAS benchmarks have
 considerable amount of communications embedded in these programs. During the

-communication process the processor remain idle until the communication has
+communication process the processors remain idle until the communication has

 finished. For that reason any change in the frequency has no impact on the time
 of communication but it has obvious impact on the time of
 finished. For that reason any change in the frequency has no impact on the time
 of communication but it has obvious impact on the time of

-computation~\cite{17}. We are made many tests on real cluster to prove that the
+computation~\cite{17}. We have made many tests on a real cluster to prove that the

 frequency scaling factor \emph S has a linear relation with computation time
 frequency scaling factor \emph S has a linear relation with computation time

-only also see~\cite{41}. To predict the execution time of MPI program, firstly
-must be precisely specifying communication time and the computation time for the
-slower task. Secondly, we use these times for predicting the execution time for
-any MPI program as a function of the new scaling factor as in the
-EQ~(\ref{eq:tnew}).
+only. To predict the execution time of MPI program, the communication time and 
+the computation time for the slower task must be first precisely specified. Secondly, 
+these times are used to predict the execution time for any MPI program as a function of 
+the new scaling factor as in the EQ~(\ref{eq:tnew}).

 \begin{equation}
   \label{eq:tnew}
 \begin{equation}
   \label{eq:tnew}

-  T_{new} = T_{\textit{Max Comp Old}} \cdot S + T_{\textit{Max Comm Old}}
+ \textit  T_\textit{new} = T_\textit{Max Comp Old} \cdot S + T_{\textit{Max Comm Old}}

 \end{equation}
 The above equation shows that the scaling factor \emph S has linear relation
 with the computation time without affecting the communication time. The
 \end{equation}
 The above equation shows that the scaling factor \emph S has linear relation
 with the computation time without affecting the communication time. The


@@ -315,7 +324,7 @@ communication time consists of the beginning times which an MPI calls for
 sending or receiving till the message is synchronously sent or received. In this
 paper we predict the execution time of the program for any new scaling factor
 value. Depending on this prediction we can produce our energy-performance scaling
 sending or receiving till the message is synchronously sent or received. In this
 paper we predict the execution time of the program for any new scaling factor
 value. Depending on this prediction we can produce our energy-performance scaling

-method as we will show in the coming sections. In the next section we make an
+method as we will show in the coming sections. In the next section we make to finishan

 investigation study for the EQ~(\ref{eq:tnew}).
 
 \section{Performance Prediction Verification}
 investigation study for the EQ~(\ref{eq:tnew}).
 
 \section{Performance Prediction Verification}


@@ -343,7 +352,7 @@ In our cluster there are 18 available frequency states for each processor from
 2.5 GHz to 800 MHz, there is 100 MHz difference between two successive
 frequencies. For more details on the characteristics of the platform refer to
 table~(\ref{table:platform}). This lead to 18 run states for each program. We
 2.5 GHz to 800 MHz, there is 100 MHz difference between two successive
 frequencies. For more details on the characteristics of the platform refer to
 table~(\ref{table:platform}). This lead to 18 run states for each program. We

-use seven MPI programs of the NAS parallel benchmarks : CG, MG, EP, FT, BT, LU
+use seven MPI programs of the NAS parallel benchmarks: CG, MG, EP, FT, BT, LU

 and SP. The average normalized errors between the predicted execution time and
 the real time (SimGrid time) for all programs is between 0.0032 to 0.0133. AS an
 example, we are present the execution times of the NAS benchmarks as in the
 and SP. The average normalized errors between the predicted execution time and
 the real time (SimGrid time) for all programs is between 0.0032 to 0.0133. AS an
 example, we are present the execution times of the NAS benchmarks as in the


@@ -361,29 +370,22 @@ it is linear see~\cite{17}. The relation between the energy and the performance
 is not straightforward. Moreover, they are not measured using the same metric.
 For solving this problem, we normalize the energy by calculating the ratio
 between the consumed energy with scaled frequency and the consumed energy
 is not straightforward. Moreover, they are not measured using the same metric.
 For solving this problem, we normalize the energy by calculating the ratio
 between the consumed energy with scaled frequency and the consumed energy

-without scaled frequency :
+without scaled frequency:

 \begin{multline}
   \label{eq:enorm}
 \begin{multline}
   \label{eq:enorm}

-  E_\textit{Norm} = \frac{E_{Reduced}}{E_{Original}}\\
-  {} = \frac{ P_{dyn} \cdot S_i^{-2} \cdot
+  E_\textit{Norm} = \frac{ E_\textit{Reduced}}{E_\textit{Original}} \\
+        {} = \frac{P_\textit{dyn} \cdot S_i^{-2} \cdot

                \left( T_1 + \sum_{i=2}^{N}\frac{T_i^3}{T_1^2}\right) +
                \left( T_1 + \sum_{i=2}^{N}\frac{T_i^3}{T_1^2}\right) +

-               P_{static} \cdot T_1 \cdot S_i \cdot N  }{
-              P_{dyn} \cdot \left(T_1+\sum_{i=2}^{N}\frac{T_i^3}{T_1^2}\right) +
-              P_{static} \cdot T_1 \cdot N }
+               P_\textit{static} \cdot T_1 \cdot S_i \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 }

 \end{multline}
 \end{multline}

-\AG{Use \texttt{\textbackslash{}text\{xxx\}} or
-  \texttt{\textbackslash{}textit\{xxx\}} for all subscripted words in equations
-  (e.g. \mbox{\texttt{E\_\{\textbackslash{}text\{Norm\}\}}}).
-
-  Don't hesitate to define new commands :
-  \mbox{\texttt{\textbackslash{}newcommand\{\textbackslash{}ENorm\}\{E\_\{\textbackslash{}text\{Norm\}\}\}}}
-}
-By the same way we can normalize the performance as follows :
+By the same way we can normalize the performance as follows:

 \begin{equation}
   \label{eq:pnorm}
 \begin{equation}
   \label{eq:pnorm}

-  P_{Norm} = \frac{T_{New}}{T_{Old}}
-          = \frac{T_{\textit{Max Comp Old}} \cdot S +
-              T_{\textit{Max Comm Old}}}{T_{Old}}
+  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{Old}}

 \end{equation}
 The second problem is the optimization operation for both energy and performance
 is not in the same direction. In other words, the normalized energy and the
 \end{equation}
 The second problem is the optimization operation for both energy and performance
 is not in the same direction. In other words, the normalized energy and the


@@ -399,20 +401,20 @@ paper we are present a method to find the optimal scaling factor \emph S for
 optimize both energy and performance simultaneously without adding big
 overheads.  Our solution for this problem is to make the optimization process
 have the same direction. Therefore, we inverse the equation of normalize
 optimize both energy and performance simultaneously without adding big
 overheads.  Our solution for this problem is to make the optimization process
 have the same direction. Therefore, we inverse the equation of normalize

-performance as follows :
+performance as follows:

 \begin{equation}
   \label{eq:pnorm_en}
 \begin{equation}
   \label{eq:pnorm_en}

-  P^{-1}_{Norm} = \frac{T_{Old}}{T_{New}}
-               = \frac{T_{Old}}{T_{\textit{Max Comp Old}} \cdot S +
-                 T_{\textit{Max Comm Old}}}
+  P^{-1}_\textit{Norm} = \frac{ T_\textit{Old}}{ T_\textit{New}}
+               = \frac{ T_\textit{Old}}{T_\textit{Max Comp Old} \cdot S +
+                 T_\textit{Max Comm Old}}

 \end{equation}
 \begin{figure*}
   \centering
   \subfloat[Converted Relation.]{%
 \end{equation}
 \begin{figure*}
   \centering
   \subfloat[Converted Relation.]{%

-    \includegraphics[width=.33\textwidth]{file.eps}\label{fig:r1}}%
+    \includegraphics[width=.4\textwidth]{file.eps}\label{fig:r1}}%

   \qquad%
   \subfloat[Real Relation.]{%
   \qquad%
   \subfloat[Real Relation.]{%

-    \includegraphics[width=.33\textwidth]{file3.eps}\label{fig:r2}}
+    \includegraphics[width=.4\textwidth]{file3.eps}\label{fig:r2}}

   \label{fig:rel}
   \caption{The Energy and Performance Relation}
 \end{figure*}
   \label{fig:rel}
   \caption{The Energy and Performance Relation}
 \end{figure*}


@@ -424,15 +426,15 @@ in the same time, see figure~(\ref{fig:r1}). Then our objective function has the
 following form:
 \begin{equation}
   \label{eq:max}
 following form:
 \begin{equation}
   \label{eq:max}

-  \textit{MaxDist} = \max (\overbrace{P^{-1}_{Norm}}^{\text{Maximize}} -
-                           \overbrace{E_{Norm}}^{\text{Minimize}} )
+  \textit{MaxDist} = \max (\overbrace{P^{-1}_\textit{Norm}}^{\text{Maximize}} -
+                           \overbrace{E_\textit{Norm}}^{\text{Minimize}} )

 \end{equation}
 Then we can select the optimal scaling factor that satisfy the
 EQ~(\ref{eq:max}).  Our objective function can works with any energy model or
 static power values stored in a data file. Moreover, this function works in
 optimal way when the energy function has a convex form with frequency scaling
 factor as shown in~\cite{15,3,19}. Energy measurement model is not the
 \end{equation}
 Then we can select the optimal scaling factor that satisfy the
 EQ~(\ref{eq:max}).  Our objective function can works with any energy model or
 static power values stored in a data file. Moreover, this function works in
 optimal way when the energy function has a convex form with frequency scaling
 factor as shown in~\cite{15,3,19}. Energy measurement model is not the

-objective of this paper and we choose Rauber's model as an example with two
+objective of this paper and we choose Rauber and Rünger model as an example with two

 reasons that mentioned before.
 
 \section{Optimal Scaling Factor for Performance and Energy}
 reasons that mentioned before.
 
 \section{Optimal Scaling Factor for Performance and Energy}


@@ -441,7 +443,7 @@ reasons that mentioned before.
 In the previous section we described the objective function that satisfy our
 goal in discovering optimal scaling factor for both performance and energy at
 the same time. Therefore, we develop an energy to performance scaling algorithm
 In the previous section we described the objective function that satisfy our
 goal in discovering optimal scaling factor for both performance and energy at
 the same time. Therefore, we develop an energy to performance scaling algorithm

-(EPSA). This algorithm is simple and has a direct way to calculate the optimal
+($EPSA$). This algorithm is simple and has a direct way to calculate the optimal

 scaling factor for both energy and performance at the same time.
 \begin{algorithm}[tp]
   \caption{EPSA}
 scaling factor for both energy and performance at the same time.
 \begin{algorithm}[tp]
   \caption{EPSA}


@@ -455,10 +457,11 @@ scaling factor for both energy and performance at the same time.
     \For {$i=1$   to   $P_{states} $}
       \State - Calculate the new frequency as $F_{new}=F_{new} - F_{diff} $
       \State - Calculate the scale factor $S$ as in EQ~(\ref{eq:s}).
     \For {$i=1$   to   $P_{states} $}
       \State - Calculate the new frequency as $F_{new}=F_{new} - F_{diff} $
       \State - Calculate the scale factor $S$ as in EQ~(\ref{eq:s}).

-      \State - Calculate all available scales $S_i$  depend on $S$ as in EQ~(\ref{eq:si}).
-      \State - Select the maximum scale factor $S_1$ from the set of scales $S_i$.
-      \State - Calculate the normalize energy $E_{Norm}=E_{R}/E_{O}$ as in EQ~(\ref{eq:enorm}).
-      \State - Calculate the normalize inverse of performance\par
+      \State - Calculate all available scales $S_i$  depend on $S$ as\par\hspace{1 pt} in EQ~(\ref{eq:si}).
+      \State - Select the maximum scale factor $S_1$ from the set\par\hspace{1 pt} of scales $S_i$.
+      \State - Calculate the normalize energy $E_{Norm}=E_{R}/E_{O}$ 
+               \par\hspace{1 pt}  as in EQ~(\ref{eq:enorm}).
+      \State - Calculate the normalize inverse of performance\par\hspace{1 pt}

                $P_{NormInv}=T_{old}/T_{new}$ as in EQ~(\ref{eq:pnorm_en}).
       \If{  $(P_{NormInv}-E_{Norm} > Dist$) }
         \State $S_{optimal} = S$
                $P_{NormInv}=T_{old}/T_{new}$ as in EQ~(\ref{eq:pnorm_en}).
       \If{  $(P_{NormInv}-E_{Norm} > Dist$) }
         \State $S_{optimal} = S$


@@ -480,18 +483,17 @@ system. The algorithm is called just one time during the execution of the
 program. The DVFS algorithm~(\ref{dvfs}) shows where and when the EPSA algorithm is called
 in the MPI program.
 %\begin{minipage}{\textwidth}
 program. The DVFS algorithm~(\ref{dvfs}) shows where and when the EPSA algorithm is called
 in the MPI program.
 %\begin{minipage}{\textwidth}

-%\AG{Use the same format as for Algorithm~\ref{EPSA}}
+%\AG{Use the same format as for Algorithm~\ref{$EPSA$}}

 
 \begin{algorithm}[tp]
   \caption{DVFS}
   \label{dvfs}
 
 \begin{algorithm}[tp]
   \caption{DVFS}
   \label{dvfs}

-  \begin{algorithmic}
+  \begin{algorithmic}[1]

  \For {$J:=1$ to $Some-Iterations \; $}
   \State -Computations Section.
    \State -Communications Section.
  \For {$J:=1$ to $Some-Iterations \; $}
   \State -Computations Section.
    \State -Communications Section.

-   \If {$(J==1)$}
-     \State -Gather all times of computation and\par
-        \State      communication from each node.
+   \If {$(J==1)$} 
+     \State -Gather all times of computation and\par\hspace{13 pt} communication from each node.

      \State -Call EPSA with these times.
      \State -Calculate the new frequency from optimal scale.
      \State -Set the new frequency to the system.
      \State -Call EPSA with these times.
      \State -Calculate the new frequency from optimal scale.
      \State -Set the new frequency to the system.


@@ -503,10 +505,10 @@ in the MPI program.
 After obtaining the optimal scale factor from the EPSA algorithm. The program
 calculates the new frequency $F_i$ for each task proportionally to its time
 value $T_i$. By substitution of the EQ~(\ref{eq:s}) in the EQ~(\ref{eq:si}), we
 After obtaining the optimal scale factor from the EPSA algorithm. The program
 calculates the new frequency $F_i$ for each task proportionally to its time
 value $T_i$. By substitution of the EQ~(\ref{eq:s}) in the EQ~(\ref{eq:si}), we

-can calculate the new frequency $F_i$ as follows :
+can calculate the new frequency $F_i$ as follows:

 \begin{equation}
   \label{eq:fi}
 \begin{equation}
   \label{eq:fi}

-  F_i = \frac{F_{max} \cdot T_i}{S_{optimal} \cdot T_{max}}
+  F_i = \frac{F_\textit{max} \cdot T_i}{S_\textit{optimal} \cdot T_\textit{max}}

 \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
 \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


@@ -533,11 +535,11 @@ frequencies.
   \caption{Platform File Parameters}
   % title of Table
   \centering
   \caption{Platform File Parameters}
   % title of Table
   \centering

-  \begin{tabular}{ | l | l | l |l | l |l |l |  p{2cm} |}
+  \begin{tabular}{|*{7}{l|}}

     \hline
     Max & Min & Backbone & Backbone&Link &Link& Sharing  \\
     Freq. & Freq. & Bandwidth & Latency & Bandwidth& Latency&Policy  \\ \hline
     \hline
     Max & Min & Backbone & Backbone&Link &Link& Sharing  \\
     Freq. & Freq. & Bandwidth & Latency & Bandwidth& Latency&Policy  \\ \hline

-    2.5 &800 & 2.25 GBps &$5\times 10^{-7} s$& 1 GBps & $5\times 10^{-5}$ s&Full  \\
+    \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}
     GHz& MHz&  & & &  &Duplex  \\\hline
   \end{tabular}
   \label{table:platform}


@@ -553,7 +555,7 @@ inversed performance curves, because there are different communication features
 for each MPI program.  When there are little or not communications, the inversed
 performance curve is very close to the energy curve. Then the distance between
 the two curves is very small. This lead to small energy savings. The opposite
 for each MPI program.  When there are little or not communications, the inversed
 performance curve is very close to the energy curve. Then the distance between
 the two curves is very small. This lead to small energy savings. The opposite

-happens when there are a lot of communication, the distance between the two
+happens when there are a lot of communication, theto finish distance between the two

 curves is big.  This lead 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 the NAS
 curves is big.  This lead 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 the NAS


@@ -573,13 +575,10 @@ same time over all available scales.
   \label{fig:nas}
 \end{figure*}
 \begin{table}[htb]
   \label{fig:nas}
 \end{figure*}
 \begin{table}[htb]

-  \caption{Optimal Scaling Factors Results}
+  \caption{The EPSA Scaling Factors Results}

   % title of Table
   \centering
   % title of Table
   \centering

-  \AG{Use the same number of decimals for all numbers in a column,
-    and vertically align the numbers along the decimal points.
-    The same for all the following tables.}
-  \begin{tabular}{ | l | l | l |l | l | p{2cm} |}
+  \begin{tabular}{|l|*{4}{r|}}

     \hline
     Program & Optimal & Energy  & Performance&Energy-Perf.\\
     Name & Scaling Factor& Saving \%&Degradation \% &Distance  \\ \hline
     \hline
     Program & Optimal & Energy  & Performance&Energy-Perf.\\
     Name & Scaling Factor& Saving \%&Degradation \% &Distance  \\ \hline


@@ -590,7 +589,7 @@ same time over all available scales.
     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
     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}
+  \end{tabular}        

   \label{table:factors results}
   % is used to refer this table in the text
 \end{table}
   \label{table:factors results}
   % is used to refer this table in the text
 \end{table}


@@ -606,146 +605,146 @@ EPSA to selects smaller scaling factor values (inducing smaller energy savings).
 \section{Comparing Results}
 \label{sec.compare}
 
 \section{Comparing Results}
 \label{sec.compare}
 

-In this section, we compare our EPSA algorithm results with Rauber's
+In this section, we compare our EPSA algorithm results with Rauber and Rünger

 methods~\cite{3}. He had two scenarios, the first is to reduce energy to optimal
 level without considering the performance as in EQ~(\ref{eq:sopt}). We refer to
 methods~\cite{3}. He had two scenarios, the first is to reduce energy to optimal
 level without considering the performance as in EQ~(\ref{eq:sopt}). We refer to

-this scenario as $Rauber_{E}$. The second scenario is similar to the first
+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
 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 $Rauber_{E-P}$. The comparison is made in tables~(\ref{table:compare
+scenario as $R_{E-P}$. The comparison is made in tables~(\ref{table:compare

   Class A},\ref{table:compare Class B},\ref{table:compare Class C}). These
   Class A},\ref{table:compare Class B},\ref{table:compare Class C}). These

-tables show the results of our EPSA and Rauber's two scenarios for all the NAS
+tables show the results of our EPSA and Rauber and Rünger scenarios for all the NAS

 benchmarks programs for classes A,B and C.
 benchmarks programs for classes A,B and C.

-\begin{table*}[p]
+\begin{table}[p]

   \caption{Comparing Results for  The NAS Class A}
   % title of Table
   \centering
   \caption{Comparing Results for  The NAS Class A}
   % title of Table
   \centering

-  \begin{tabular}{ | l | l | l |l | l | l|  }
+  \begin{tabular}{|l|l|*{4}{r|}}

     \hline
     Method&Program&Factor& Energy& Performance &Energy-Perf.\\
     \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}
     \\ \hline
     % \rowcolor[gray]{0.85}

-    EPSA&CG & 1.56 &37.02 & 13.88 & 23.14\\ \hline
-    $Rauber_{E-P}$&CG &2.14 &42.77 & 25.27 & 17.50\\ \hline
-    $Rauber_{E}$&CG &2.14 &42.77&26.46&16.31\\ \hline
+    $EPSA$&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
-    $Rauber_{E-P}$&MG &2.14&34.45&31.84&2.61\\ \hline
-    $Rauber_{E}$&MG &2.14&34.48&33.65&0.80 \\ \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
-    $Rauber_{E-P}$&EP&2.05&41.45&55.67&-14.22\\ \hline
-    $Rauber_{E}$&EP&2.05&42.09&57.59&-15.50\\ \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
-    $Rauber_{E-P}$&LU&2.14&45.62&27.00&18.62 \\ \hline
-    $Rauber_{E}$&LU&2.14&45.66&33.01&12.65\\ \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
-    $Rauber_{E-P}$&BT&2.10&45.53&49.63&-4.10\\ \hline
-    $Rauber_{E}$&BT&2.10&43.93&52.86&-8.93\\ \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
-    $Rauber_{E-P}$&SP&2.11&45.62&42.52&3.10\\ \hline
-    $Rauber_{E}$&SP&2.11&45.78&43.09&2.69\\ \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
-    $Rauber_{E-P}$&FT&2.10&39.29&34.30&4.99 \\ \hline
-    $Rauber_{E}$&FT&2.10&37.56&38.21&-0.65\\ \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:compare Class A}
   % is used to refer this table in the text
   \end{tabular}
   \label{table:compare Class A}
   % is used to refer this table in the text

-\end{table*}
-\begin{table*}[p]
+\end{table}
+\begin{table}[p]

   \caption{Comparing Results for The NAS Class B}
   % title of Table
   \centering
   \caption{Comparing Results for The NAS Class B}
   % title of Table
   \centering

-  \begin{tabular}{ | l | l | l |l | l |l|  }
+  \begin{tabular}{|l|l|*{4}{r|}}

     \hline
     Method&Program&Factor& Energy& Performance &Energy-Perf.\\
     \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}
     \\ \hline
     % \rowcolor[gray]{0.85}

-    EPSA&CG & 1.66 &39.23&16.63&22.60   \\ \hline
-    $Rauber_{E-P}$&CG &2.15 &45.34&27.60&17.74\\ \hline
-    $Rauber_{E}$&CG &2.15 &45.34&28.88&16.46\\ \hline
+    $EPSA$&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
-    $Rauber_{E-P}$&MG &2.14&43.55&36.42&7.13 \\ \hline
-    $Rauber_{E}$&MG &2.14&43.56&37.07&6.49 \\ \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

 
 

-    EPSA&EP &1.08 &20.29&17.15&3.14 \\ \hline
-    $Rauber_{E-P}$&EP&2.00&42.38&56.88&-14.50\\ \hline
-    $Rauber_{E}$&EP&2.00&39.73&59.94&-20.21\\ \hline
+    $EPSA$&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
-    $Rauber_{E-P}$&LU&2.10&43.62&36.51&7.11 \\ \hline
-    $Rauber_{E}$&LU&2.10&43.61&38.54&5.07 \\ \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
-    $Rauber_{E-P}$&BT&2.10&44.53&53.05&-8.52\\ \hline
-    $Rauber_{E}$&BT&2.10&42.93&52.80&-9.87\\ \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
-    $Rauber_{E-P}$&SP&2.15&45.69&43.20&2.49\\ \hline
-    $Rauber_{E}$&SP&2.15&45.41&44.47&0.94\\ \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
-    $Rauber_{E-P}$&FT&2.13&42.98&37.35&5.63 \\ \hline
-    $Rauber_{E}$&FT&2.13&43.04&37.90&5.14\\ \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:compare Class B}
   % is used to refer this table in the text
   \end{tabular}
   \label{table:compare Class B}
   % is used to refer this table in the text

-\end{table*}
+\end{table}

 
 

-\begin{table*}[p]
+\begin{table}[p]

   \caption{Comparing Results for The NAS Class C}
   % title of Table
   \centering
   \caption{Comparing Results for The NAS Class C}
   % title of Table
   \centering

-  \begin{tabular}{ | l | l | l |l | l |l|  }
+  \begin{tabular}{|l|l|*{4}{r|}}

     \hline
     Method&Program&Factor& Energy& Performance &Energy-Perf.\\
     \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}
     \\ \hline
     % \rowcolor[gray]{0.85}

-    EPSA&CG & 1.56 &39.23&14.88&24.35  \\ \hline
-    $Rauber_{E-P}$&CG &2.15 &45.36&25.89&19.47\\ \hline
-    $Rauber_{E}$&CG &2.15 &45.36&26.70&18.66\\ \hline
+    $EPSA$&CG & 1.56 &39.23&14.88&24.35  \\ \hline
+    $R_{E-P}$&CG &2.15 &45.36&25.89&19.47\\ \hline
+    $R_{E}$&CG &2.15 &45.36&26.70&18.66\\ \hline

 
 

-    EPSA&MG & 1.47 &34.97&21.69&13.27\\ \hline
-    $Rauber_{E-P}$&MG &2.15&43.65&40.45&3.20 \\ \hline
-    $Rauber_{E}$&MG &2.15&43.64&41.38&2.26 \\ \hline
+    $EPSA$&MG & 1.47 &34.97&21.69&13.27\\ \hline
+    $R_{E-P}$&MG &2.15&43.65&40.45&3.20 \\ \hline
+    $R_{E}$&MG &2.15&43.64&41.38&2.26 \\ \hline

 
 

-    EPSA&EP &1.04 &22.14&20.73&1.41 \\ \hline
-    $Rauber_{E-P}$&EP&1.92&39.40&56.33&-16.93\\ \hline
-    $Rauber_{E}$&EP&1.92&38.10&56.35&-18.25\\ \hline
+    $EPSA$&EP &1.04 &22.14&20.73&1.41 \\ \hline
+    $R_{E-P}$&EP&1.92&39.40&56.33&-16.93\\ \hline
+    $R_{E}$&EP&1.92&38.10&56.35&-18.25\\ \hline

 
 

-    EPSA&LU&1.38&35.83&22.49&13.34 \\ \hline
-    $Rauber_{E-P}$&LU&2.15&44.97&41.00&3.97 \\ \hline
-    $Rauber_{E}$&LU&2.15&44.97&41.80&3.17 \\ \hline
+    $EPSA$&LU&1.38&35.83&22.49&13.34 \\ \hline
+    $R_{E-P}$&LU&2.15&44.97&41.00&3.97 \\ \hline
+    $R_{E}$&LU&2.15&44.97&41.80&3.17 \\ \hline

 
 

-    EPSA&BT&1.31& 29.60&21.28&8.32\\ \hline
-    $Rauber_{E-P}$&BT&2.13&45.60&49.84&-4.24\\ \hline
-    $Rauber_{E}$&BT&2.13&44.90&55.16&-10.26\\ \hline
+    $EPSA$&BT&1.31& 29.60&21.28&8.32\\ \hline
+    $R_{E-P}$&BT&2.13&45.60&49.84&-4.24\\ \hline
+    $R_{E}$&BT&2.13&44.90&55.16&-10.26\\ \hline

 
 

-    EPSA&SP&1.38&33.48&21.35&12.12\\ \hline
-    $Rauber_{E-P}$&SP&2.10&45.69&43.60&2.09\\ \hline
-    $Rauber_{E}$&SP&2.10&45.75&44.10&1.65\\ \hline
+    $EPSA$&SP&1.38&33.48&21.35&12.12\\ \hline
+    $R_{E-P}$&SP&2.10&45.69&43.60&2.09\\ \hline
+    $R_{E}$&SP&2.10&45.75&44.10&1.65\\ \hline

 
 

-    EPSA&FT&1.47&34.72&19.00&15.72 \\ \hline
-    $Rauber_{E-P}$&FT&2.04&39.40&37.10&2.30\\ \hline
-    $Rauber_{E}$&FT&2.04&39.35&37.70&1.65\\ \hline
+    $EPSA$&FT&1.47&34.72&19.00&15.72 \\ \hline
+    $R_{E-P}$&FT&2.04&39.40&37.10&2.30\\ \hline
+    $R_{E}$&FT&2.04&39.35&37.70&1.65\\ \hline

   \end{tabular}
 \label{table:compare Class C}
 % is used to refer this table in the text
   \end{tabular}
 \label{table:compare Class C}
 % is used to refer this table in the text

-\end{table*}
+\end{table}

 As shown in these tables our scaling factor is not optimal for energy saving
 such as Rauber's scaling factor EQ~(\ref{eq:sopt}), but it is optimal for both
 As shown in these tables our scaling factor is not optimal for energy saving
 such as Rauber's scaling factor EQ~(\ref{eq:sopt}), but it is optimal for both

-the energy and the performance simultaneously. Our EPSA optimal scaling factors
+the energy and the performance simultaneously. Our $EPSA$ optimal scaling factors

 has better simultaneous optimization for both the energy and the performance
 has better simultaneous optimization for both the energy and the performance

-compared to Rauber's energy-performance method ($Rauber_{E-P}$). Also, in
-($Rauber_{E-P}$) method when setting the frequency to maximum value for the
+compared to Rauber and Rünger energy-performance method ($R_{E-P}$). Also, in
+($R_{E-P}$) method when setting the frequency to maximum value for the

 slower task lead to a small improvement of the performance. Also the results
 show that this method keep or improve energy saving. Because of the energy
 consumption decrease when the execution time decreased while the frequency value
 slower task lead to a small improvement of the performance. Also the results
 show that this method keep or improve energy saving. Because of the energy
 consumption decrease when the execution time decreased while the frequency value


@@ -754,8 +753,8 @@ increased.
 Figure~(\ref{fig:compare}) shows the maximum distance between the energy saving
 percent and the performance degradation percent. Therefore, this means it is the
 same resultant of our objective function EQ~(\ref{eq:max}). Our algorithm always
 Figure~(\ref{fig:compare}) shows the maximum distance between the energy saving
 percent and the performance degradation percent. Therefore, this means it is the
 same resultant of our objective function EQ~(\ref{eq:max}). Our algorithm always

-gives positive energy to performance trade offs while Rauber's method
-($Rauber_{E-P}$) gives in some time negative trade offs such as in BT and
+gives positive energy to performance trade offs while Rauber and Rünger method
+($R_{E-P}$) gives in some time negative trade offs such as in BT and

 EP. The positive trade offs with highest values lead to maximum energy savings
 concatenating with less performance degradation and this the objective of this
 paper. While the negative trade offs refers to improving energy saving (or may
 EP. The positive trade offs with highest values lead to maximum energy savings
 concatenating with less performance degradation and this the objective of this
 paper. While the negative trade offs refers to improving energy saving (or may


@@ -766,20 +765,22 @@ than the first.
   \includegraphics[width=.33\textwidth]{compare_class_A.pdf}
   \includegraphics[width=.33\textwidth]{compare_class_B.pdf}
   \includegraphics[width=.33\textwidth]{compare_class_c.pdf}
   \includegraphics[width=.33\textwidth]{compare_class_A.pdf}
   \includegraphics[width=.33\textwidth]{compare_class_B.pdf}
   \includegraphics[width=.33\textwidth]{compare_class_c.pdf}

-  \caption{Comparing Our EPSA with Rauber's Methods}
+  \caption{Comparing Our EPSA with Rauber and Rünger Methods}

   \label{fig:compare}
 \end{figure}
   \label{fig:compare}
 \end{figure}

-

 \section{Conclusion}
 \label{sec.concl}
 \section{Conclusion}
 \label{sec.concl}

-
-\AG{the conclusion needs to be written\dots{} one day}
+In this paper we develop the simultaneous energy-performance algorithm. It is works based on the trade off relation between the energy and performance. The results showed that when the scaling factor is big value leads to more energy saving. Also, it show that when the the scaling factor is small value leads to the fact that the scaling factor has bigger impact on performance than energy. Then the algorithm optimize the energy saving and performance in the same time to have positive trade off. The optimal trade off refer to maximum distance between the energy and the inversed performance curves. Also, the results explained when setting the slowest task to maximum frequency usually not have a big improvement on performance. 

 
 \section*{Acknowledgment}
 
 \AG{Right?}
 Computations have been performed on the supercomputer facilities of the
 Mésocentre de calcul de Franche-Comté.
 
 \section*{Acknowledgment}
 
 \AG{Right?}
 Computations have been performed on the supercomputer facilities of the
 Mésocentre de calcul de Franche-Comté.

+As a PhD student, M. Ahmed Fanfakh, would like to thank the University of
+Babylon (Iraq) for supporting his scholarship program that allows him to work on
+this paper.
+\AG{What about simply: ``[...] for supporting his work.''}

 
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 % trigger a \newpage just before the given reference
 % number - used to balance the columns on the last page


@@ -798,5 +799,5 @@ Mésocentre de calcul de Franche-Comté.
 %%% ispell-local-dictionary: "american"
 %%% End:
 
 %%% ispell-local-dictionary: "american"
 %%% End:
 

-%  LocalWords:  Badri Charr FIXME Tianhe DVFS HPC NAS NPB SMPI Rauber's Rauber
-%  LocalWords:  CMOS EQ EPSA Franche Comté Tflop
+%  LocalWords:  Fanfakh Charr FIXME Tianhe DVFS HPC NAS NPB SMPI Rauber's Rauber
+%  LocalWords:  CMOS EQ EPSA Franche Comté Tflop Rünger