From 0465f42aaa2cd6ca1b5a122e6461818f309140c2 Mon Sep 17 00:00:00 2001 From: lilia Date: Mon, 28 Apr 2014 17:51:43 +0200 Subject: [PATCH] v10 --- hpcc.tex | 6 +++--- 1 file changed, 3 insertions(+), 3 deletions(-) diff --git a/hpcc.tex b/hpcc.tex index 371c1ed..2bb3997 100644 --- a/hpcc.tex +++ b/hpcc.tex @@ -493,7 +493,7 @@ simulates the case of distant clusters linked with long distance network as in g Both codes were simulated on a two clusters based network with 50 hosts each, totaling 100 hosts. Various combinations of the above -factors have provided the results shown in Table~\ref{tab.cluster.2x50}. The problem size of the 3D Poisson problem ranges from $N_x = N_y = N_z = \text{62}$ to 150 elements (that is from +factors have provided the results shown in Table~\ref{tab.cluster.2x50}. The problem size of the 3D Poisson problem ranges from $N=N_x = N_y = N_z = \text{62}$ to 150 elements (that is from $\text{62}^\text{3} = \text{\np{238328}}$ to $\text{150}^\text{3} = \text{\np{3375000}}$ entries). With the asynchronous multisplitting algorithm the simulated execution time is in average 2.5 times faster than with the synchronous GMRES one. %\AG{Expliquer comment lire les tableaux.} @@ -523,7 +523,7 @@ $\text{62}^\text{3} = \text{\np{238328}}$ to $\text{150}^\text{3} = power (GFlops) & 1 & 1 & 1 & 1.5 & 1.5 \\ \hline - size $(n^3)$ + size $(N)$ & 62 & 62 & 62 & 100 & 100 \\ \hline Precision @@ -548,7 +548,7 @@ $\text{62}^\text{3} = \text{\np{238328}}$ to $\text{150}^\text{3} = Power (GFlops) & 1.5 & 1.5 & 1.5 & 1.5 & 1.5 \\ % & 1 & 1.5 \\ \hline - size $(n^3)$ + size $(N)$ & 110 & 120 & 130 & 140 & 150 \\ % & 171 & 171 \\ \hline Precision -- 2.39.5