X-Git-Url: https://bilbo.iut-bm.univ-fcomte.fr/and/gitweb/mpi-energy2.git/blobdiff_plain/6f654dc78519e3caa1dfdec3a8be444277823ce4..880d3292a3cbcef0558f76eb03b22722e9e31db0:/mpi-energy2-extension/review/review.tex diff --git a/mpi-energy2-extension/review/review.tex b/mpi-energy2-extension/review/review.tex index d49b795..a7253f6 100644 --- a/mpi-energy2-extension/review/review.tex +++ b/mpi-energy2-extension/review/review.tex @@ -187,7 +187,9 @@ For the variability issue, please refer to the answer to question 1. \section{Questions and remarks of the second reviewer} \begin{enumerate} -\item Move the contributions from related work to introduction +\item Move the contributions from related work to introduction. + +\textbf{Answer:} The contributions were moved to the introduction section. \item Why emphasize it is a grid platform? the presentation of related work follows the logic of heterogeneous CPUs. Grid is only a type of platform with heterogeneous CPUs. @@ -273,13 +275,16 @@ by the scheduler of the operating system of the node. \item Why $T_{old}$ is computed using eq. 12, which applies MAX over computation time and communication time, while in $T_{new}$, max and min operations are applied over computation and communication separately? -\textcolor{blue}{Answer: We agree with the reviewer, $T_{old}$ is the maximum execution time of the application before scaling the frequency and it is computed as in $T_{new}$ equation without scaling factors. So, we have changed the $T_{old}$ in the paper as as follows: +\textbf{Answer:} Both forms can be used for computing $T_{old}$ and $T_{new}$. To avoid this confusion, the same form was used for both equations in the paper. + \begin{equation} \label{eq:told} T_{old} = \mathop{\max_{i=1,2,\dots,N}}_{j=1,2,\dots,M_i} (\Tcp[ij]) + - \mathop{\min_{i=1,2,\dots,N}} (\Tcm[hj] ) + \mathop{\min_{j=1,2,\dots,M_h}} (\Tcm[hj] ) \end{equation} -} +where $h$ is the index of the slowest cluster. + + \item Line 55 on page 16 is to define the slack time, which should be introduced at the beginning of the paper, such as in figure 1.