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@jemoka / Jemoka Knowledge Base / raw/course/math53_practice/kbhsu_math53_practice_1_problem_4.md
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--- title: "SU-MATH53 Practice 1 Problem 4" source: https://www.jemoka.com/posts/kbhsu_math53_practice_1_problem_4/ --- We have: \begin{equation} \pdv[2]{u}{x} + \pdv[2]{u}{y} = 0 \end{equation} Ignoring the boundary conditions when \(u(0,y)\), we know that we have Dirichlet boundaries in \(y\). This gives: \begin{equation} u(x,0) = u(x,\pi) = 0 \end{equation} Assuming our solution takes on the shape of \(u=X(x)Y(y)\), we obtain: \begin{equation} X’’(x)Y(y) + Y’’(y)X(x) = 0 \end{equation} by plugging in derivatives of that assumption; meaning: \begin{equation} X’’(x)Y(y) = -Y’’(y)X(x) \end{equation} This gives rise to: \begin{align} \frac{X’’(x)}{X(x)} = -\frac{Y’’(y)}{Y(y)} = c \end{align} [you know why \(c>0\), so let’s skip to] We have \(c>0\), meaning: \begin{equation} X’’(x) = cX(x) \end{equation} for some positive \(c\); this will result in a linear combination of exponentials: \begin{equation} X(x) = a_{1} e^{\sqrt{c}x} + a_2 e^{-\sqrt{c}x} \end{equation} this is because… try it! try solving \(X’’(x) = cX(x)\). Now, importantly, let’s declare: \begin{equation} \lambda = \sqrt{c} \end{equation} This gives: \begin{equation} c = \lambda^{2} \end{equation} Meaning, we have: \begin{equation} \frac{Y’’(y)}{Y(y)} = -\lambda^{2} \end{equation} meaning: \begin{equation} Y’’(y) = -\lambda^{2} Y(y) \end{equation} Now, given we now have a negative sign in front of our second order ODE, we can see that this falls into the sinusoid case, whereby: \begin{equation} Y = a_3 \cos \qty(\lambda x) + a_4 \sin \qty(\lambda x) \end{equation} Our boundary condition gives: \begin{equation} Y_0 = Y_{\pi} = 0 = a_3 = 0 \end{equation} meaning \begin{equation} Y = a_4 \sin \qty(\lambda x) \end{equation} and so on. You multiply them together and all’s well that ends well.