I wish to obtain the eigenfunctions/eigenvalues of $\nabla^2 \phi(x,y) +\lambda \phi(x,y) = 0$ with boundary conditions $\phi(x,0) = \phi(x,\pi) = \phi(0,y) = \phi(\pi,y) = 0$. To do this, I consider the method of Separation of Variables.
Ansatz: $\phi = X(x)Y(y)$. Then substituting appropriately I obtain: $$ \frac{X''}{X} = -\frac{(Y'' + \lambda Y)}{Y} = -\mu $$ which yields the two equations $$\begin{cases}X'' + \mu X &= 0 \\ Y'' + (\lambda - \mu)Y &=0\end{cases}$$ and corresponding boundary conditions: $$X(x)Y(0) = X(x)Y(\pi) = X(0)Y(y) = X(\pi)Y(y) = 0$$
Questions:
- In the equation for $X$ the variable $-\mu$ is called the eigenvalue of the $X$ equation because we can write $DX = -\mu X$ where $D := \partial_x^2$ and so $-\mu$ is an eigenvalue of this equation. For the $Y$ equation the eigenvalue is $-(\lambda - \mu )$. If I find the values for $\lambda, \mu$ then...what does this mean for the original problem. Is the product of the eigenfunctions of the respective equations again an eigenfunction for the original problem?
- I have issue actually solving this system of equations with the boundary conditions. From my observation it does not seem possible to solve for the four coefficients the result from solving the equations. See below:
Solving the $X$ equation I obtain: $X = c_1 \cos(\sqrt(\mu)x)+c_2\sin(\sqrt{\mu}x)$
Solving the $Y$ equation I obtain $Y = c_3\cos(\sqrt{(\lambda - \mu)}y) + c_4\sin(\sqrt{(\lambda-\mu)}y)$
I obtain $c_1 = c_3 = 0$. But now I have the equations $$\begin{cases}c_2\sin(\sqrt{\mu}x)c_4\sin(\sqrt{(\lambda-\mu)}\pi) &=0 \\ c_2\sin(\sqrt{\mu}\pi)c_4 \sin(\sqrt{(\lambda-\mu)}y) &= 0\end{cases}$$
Correct?
– hirotaFan Mar 30 '21 at 19:33