Merge branch 'janitaws/latex' of github.uio.no:FYS3150-G2-2023/Project-4 into janitaws/latex

This commit is contained in:
Cory Balaton 2023-12-05 18:17:44 +01:00
commit b84994f1fb
No known key found for this signature in database
GPG Key ID: 3E5FCEBFD80F432B

View File

@ -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 balance, compared to the OpenMP load balance. The master process gatheres all the
data using blocking communication, resulting in the other processes waiting. This 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 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 In Figure \ref{fig:phase_energy_10M}, for the larger lattices we observe a sharper
increase in $\langle \epsilon \rangle$ in the temperature range $T \in [2.25, 2.35]$. %] 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 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 estimate with the analytical solution, the relative error of our estimate is
\begin{equation*} \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{equation*}
\end{document} \end{document}