For the stated problem I got the following equations after applying separation of variables, I am confused as to how to apply the mentioned boundary conditions to this problem :
\begin{align} G''(x)+(4\pi^2-c)G(x)&=0\\ 4H''(y)+cH(y)&=0 \end{align}
For the stated problem I got the following equations after applying separation of variables, I am confused as to how to apply the mentioned boundary conditions to this problem :
\begin{align} G''(x)+(4\pi^2-c)G(x)&=0\\ 4H''(y)+cH(y)&=0 \end{align}
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For the first part...I'm calling $c$ lambda $\lambda$
$$ G^{''}(x) + (4\pi^{2} - \lambda )G(x) = 0 \tag{1} $$
call $4\pi^{2} - \lambda = \alpha $
$$ G^{''}(x) + \alpha G(x) = 0 \tag{2} $$
$$ G(x) = c_{1} \cos(\sqrt{\alpha}x) + c_{2}\sin(\sqrt{\alpha}x) \tag{3} $$
the x boundaries are neumann
$$ \frac{\partial }{\partial x}G(x) = -\sqrt{\alpha}c_{1}\sin(\sqrt{\alpha}x) + \sqrt{\alpha}c_{2}\cos(\sqrt{\alpha}x) \tag{4} $$
put in $x=0$ and $c_{2} =0$
$$ \frac{\partial }{\partial x}G(0) = \sqrt{\alpha}c_{2} = 0\tag{5} $$
now $G(x) = c_{1}\cos(\sqrt{\alpha}x) $
$$ \frac{\partial }{\partial x}G(1) = -\sqrt{\alpha}c_{1}\sin(\sqrt{\alpha}1) = \sin(\sqrt{\alpha}) \tag{6} $$
in order to determine the eigenvalues, is this good? Can you apply the $y$ boundaries now?
Note for the next one you have
$$ H^{''}(y) + \frac{\lambda}{4}H(y) = 0 \tag{7} $$
however, the eigenvalues are going to be related now
Edit
If you simply solve the above on line $6$ and we let the boundary actually be $L$
$$\sin(\sqrt{\alpha}L) = 0 \implies \sqrt{\alpha}L = n\pi \implies \sqrt{\alpha} = \frac{n\pi}{L} \tag{8} $$
now remember what $\alpha$ is
$$ \sqrt{\alpha} = \sqrt{4\pi^{2} - \lambda} =\frac{n\pi}{L} \tag{9} $$
now $L =1$
$$4\pi^{2} - \lambda =n^{2}\pi^{2} \tag{10}$$
$$ - \lambda = n^{2}\pi^{2} - 4\pi^{2} \implies \lambda = 4\pi^{2} - n^{2}\pi^{2} \tag{11}$$