From f3324e0a747b849aecd9a0c813c697cd5b3ee5e2 Mon Sep 17 00:00:00 2001 From: Sam0h51 <75147348+Sam0h51@users.noreply.github.com> Date: Mon, 19 Feb 2024 11:55:32 -0700 Subject: [PATCH] Update README.md --- Swift-Hohenberg-Solver/README.md | 10 ++++++++-- 1 file changed, 8 insertions(+), 2 deletions(-) diff --git a/Swift-Hohenberg-Solver/README.md b/Swift-Hohenberg-Solver/README.md index e3b8969..3a5ac6e 100755 --- a/Swift-Hohenberg-Solver/README.md +++ b/Swift-Hohenberg-Solver/README.md @@ -1,3 +1,9 @@ +--- +title: "Swift-Hohenberg Solver Write-up" +bibliography: references.bib +link-citations: true +--- + # Introduction This program is used to solve the generalized Swift-Hohenberg equation @@ -15,7 +21,7 @@ wavelength of $2\pi$. We choose $r = 0.3$ because solutions are reasonably well behaved for small values of $r$ and $g_1$, but there are interesting behaviors that occur when $g_1$ is smaller or larger than $r$ in magnitude, so this allows us room to vary $g_1$ and -explore these behavior. To summarize, this code solves: +explore these behavior. Additionally, we choose $r = 0.3$ because this matches the parameters used by Gurevich in \cite{Gurevich}. We chose our parameters to match so that we could compare the output of our program to the results presented in \cite{Gurevich}, which was useful for validating that our code was functioning properly during the developement process. To summarize, this code solves: @f{align*}{ \frac{\partial u}{\partial t} = 0.3u - (1 + \Delta)^2 u + g_1 u^2 - u^3 @@ -259,4 +265,4 @@ patterns that form. Each image sequence was taken at times 0, 10, 25, ![image](./doc/images/Sphere_Random_Table.png) -![image](./doc/images/Sinusoid_Random_Table.png) \ No newline at end of file +![image](./doc/images/Sinusoid_Random_Table.png) -- 2.39.5