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[SOLVED] orthogonal eigenfunctions
From Sturm-Louisville eigenvalue theory we know that eigenfunctions corresponding to different eigenvalues are orthogonal. For example,
\Phi_{xx} + \lambda \Phi = 0
would be of Sturm-Louisville form (note: \Phi_{xx} represents the second derivative of Phi with respect to x)
\frac{d}{dx}[p(x) \frac{d \Phi}{dx}] + (q(x) + \sigma(x) \lambda)\Phi = 0
where q = 0, p = 1, and \sigma = 1. The boundary conditions are
BC1: \Phi(0) = 0
and
BC2: \Phi_x(L) + h \Phi(L,t) = 0
which means that there can be one eigenfunction corresponding to a negative eigenvalue and the rest are sines relating to the positive eigenvalues, specifically that the eigenfunctions would be
\Phi_n(x) = \left\{ {\begin{array}{*{20}c}<br /> {sinh \sqrt{s_1}x} & {n=1} \\<br /> {sin\sqrt{\lambda_n}x} & {n > 1} \\<br /> \end{array}} \right.
Basically all I need to do is show that
\int_0^L sin \sqrt{\lambda_n}x sinh \sqrt{s_1} x dx = 0
with integration by parts I have gotten to the point
\int_0^L sin \sqrt{\lambda_n}x sinh \sqrt{s_1} x dx = \frac{\sqrt{s_e}cosh(\sqrt{s_e}L)sin(L\sqrt{\lambda}) - \sqrt{\lambda_n}cos(\sqrt{\lambda_n}L)sinh(L\sqrt{s_e})}{s_e+\lambda}
and mathematica gives the same thing. I don't see this being zero any time soon. Any suggestions?
From Sturm-Louisville eigenvalue theory we know that eigenfunctions corresponding to different eigenvalues are orthogonal. For example,
\Phi_{xx} + \lambda \Phi = 0
would be of Sturm-Louisville form (note: \Phi_{xx} represents the second derivative of Phi with respect to x)
\frac{d}{dx}[p(x) \frac{d \Phi}{dx}] + (q(x) + \sigma(x) \lambda)\Phi = 0
where q = 0, p = 1, and \sigma = 1. The boundary conditions are
BC1: \Phi(0) = 0
and
BC2: \Phi_x(L) + h \Phi(L,t) = 0
which means that there can be one eigenfunction corresponding to a negative eigenvalue and the rest are sines relating to the positive eigenvalues, specifically that the eigenfunctions would be
\Phi_n(x) = \left\{ {\begin{array}{*{20}c}<br /> {sinh \sqrt{s_1}x} & {n=1} \\<br /> {sin\sqrt{\lambda_n}x} & {n > 1} \\<br /> \end{array}} \right.
Basically all I need to do is show that
\int_0^L sin \sqrt{\lambda_n}x sinh \sqrt{s_1} x dx = 0
with integration by parts I have gotten to the point
\int_0^L sin \sqrt{\lambda_n}x sinh \sqrt{s_1} x dx = \frac{\sqrt{s_e}cosh(\sqrt{s_e}L)sin(L\sqrt{\lambda}) - \sqrt{\lambda_n}cos(\sqrt{\lambda_n}L)sinh(L\sqrt{s_e})}{s_e+\lambda}
and mathematica gives the same thing. I don't see this being zero any time soon. Any suggestions?