-This section presents results of applying the frequency selection algorithm \ref{EPSA} using
-the new proposed energy model \ref{eq:e-new}. The algorithm is applied to NAS parallel benchmarks class
-C running on 16 computing nodes using the SimGrid simulator. Same values are used for the static and dynamic powers values as in section \ref{ch2:6:2}. Two measured energy consumptions of the NAS benchmarks class C using the new energy model and Rauber and Rünger's model are presented in the figure \ref{fig:energy_con}. The energy consumptions of both models are computed using similar parameters: frequency scaling factors, dynamic and static powers values. As shown in this figure, the majority of the benchmarks have smaller computed energies values using the new model compare to those use Rauber and Rünger's model.
-Indeed, there are two reasons explaining these differences in the energy consumptions. The first one is related to the dynamic power consumption, where the new energy model ensures that this power metric is consumed only during the computation time, while the other model assumes to consume the dynamic power during both computation and communication times and thus more dynamic energy consumption is given.
-The second one is related to the execution time, that is only its computation times is increased with the
-scaling factor value in the new energy model, while other energy model indicates that both the
-computation and communication times are increased with scaling factor and hence more static energy consumption is given. Therefore, the MPI programs that have big communication times, they have bigger measured energy consumption values using Rauber and Rünger's model compare to the new model as in CG, SP, LU and FT benchmarks. Whereas, if the MPI programs have very small communication times, their computed energy values have very small differences such as in MG and BT benchmarks, or they are identical such as in EP benchmark where there is no communication and no idle times.
+This section presents the results of applying the frequency selection algorithm \ref{EPSA} using the new proposed energy model \ref{eq:e-new} to NAS parallel benchmarks.
+The class C of the benchmarks was executed on a homogeneous architecture composed of 16 nodes and simulated by SimGrid. The same static and dynamic power values were used as in section \ref{ch2:6:2}. Figure \ref{fig:energy_con} presents the energy consumption of the NAS benchmarks class C using the new energy model and Rauber and Rünger's model. The energy consumptions of both models are computed using similar parameters: frequency scaling factors, dynamic and static powers values. As shown in this figure, the majority of the benchmarks consumes less energy using the new model than when using Rauber and Rünger's model.
+Two reasons explain these differences in the energy consumptions: the first one is related to the dynamic power consumption, where the new energy model ensures that this power metric is only consumed during the computation time, while the other model assumes that the dynamic power is consumed during both computation and communication times and thus increasing the dynamic energy consumption.
+The second reason is related to the execution time. In the new model only the computation times are increased when the frequency of a processor is scaled down, while
+Rauber and Rünger's model indicates that both the computation and communication times
+are increased according to the scaling factor and hence more static energy is consumed. Therefore, the MPI programs that have big communication times, have bigger energy consumption values using Rauber and Rünger's model when compared to the new model as for the CG, SP, LU and FT benchmarks. Whereas, if the MPI programs have very small communication times, their computed energy values have very small differences using both models such as in MG and BT benchmarks, or they are identical such as for the EP benchmark where there is no communication and no idle times.