How to Solve a Complex 2D PDE in Toroidal Coordinates?

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maverick280857
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Hi,

After considerable simplification in a problem I'm working on, I end up with the following partial differential equation:

[tex] \partial_{\eta}\left(\frac{\sinh\eta}{\Delta}\partial_{\eta}g\right) + \partial_{\theta}\left(\frac{\sinh\eta}{\Delta}\partial_{\theta}g\right) + c^2\left[\frac{E_{p} - V(\eta,\theta)}{\Delta\sinh\eta}\right]g = 0[/tex]

where c is a positive constant, [itex]E_{p}[/itex] is a constant, [itex]V_{0}[/itex] is a constant and

[tex]V(\eta,\theta) = V_0\sqrt{\frac{\Delta}{\sinh\eta}}Q_{-1/2}(\coth\eta)[/tex]

where Q is the Legendre function,

[tex]\Delta = \cosh\eta - \cos\theta[/tex]

The d.e. actually comes from a separation of variables in toroidal coordinates. I am not sure how I should proceed to solve this differential equation for [itex]g(\eta,\theta)[/itex].

Any inputs on how to solve this differential equation analytically will be appreciated.

Thanks in advance!
 
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Is there some substitution which will simplify this equation maybe?