From 2c1c2e77b06d8b30a9b4cacfc52d61abcc92d5af Mon Sep 17 00:00:00 2001 From: Janita Willumsen Date: Tue, 5 Dec 2023 15:43:33 +0100 Subject: [PATCH] Fix tense and variable name --- latex/sections/results.tex | 4 ++-- 1 file changed, 2 insertions(+), 2 deletions(-) diff --git a/latex/sections/results.tex b/latex/sections/results.tex index 9ca95ca..45d8d3f 100644 --- a/latex/sections/results.tex +++ b/latex/sections/results.tex @@ -108,7 +108,7 @@ assessment output can be found in Appendix \ref{sec:additional_results} in Figur balance, compared to the OpenMP load balance. The master process gatheres all the data using blocking communication, resulting in the other processes waiting. This results in one process, the master, having to work more. The OpenMP load balance -score is very good, suggesting the threads are not left idle for long periods. +score is very good, suggesting that the threads are not left idle for long time periods. In Figure \ref{fig:phase_energy_10M}, for the larger lattices we observe a sharper increase in $\langle \epsilon \rangle$ in the temperature range $T \in [2.25, 2.35]$. %] @@ -187,7 +187,7 @@ of the critical temperature for a lattice of infinite size. The estimated critic is $T_{c}^{*}(L = \infty) \approx 2.2693 J/k_{B}$. We also compared the estimate with the analytical solution, the relative error of our estimate is \begin{equation*} - \text{Relative error} = \frac{T_{c}^{*} - T_{c \text{ analytical}}}{T_{c \text{ analytical}}} \approx 5.05405 \cdot 10^{-5} J/k_{B} + \text{Relative error} = \frac{T_{c}^{*} - T_{c}}{T_{c}} \approx 5.05405 \cdot 10^{-5} J/k_{B} \end{equation*} \end{document}