Two dimensional Poisson's equation, Green's function technique

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SUMMARY

The discussion centers on solving the two-dimensional Poisson's equation for a perturbed gravitational potential in a rectangular configuration, specifically involving a step function. The equation presented is (∂²/∂x² + ∂²/∂z²) ψ(x, z) = [θ(z - (a + ε cos(kx))) - θ(z - a)] + [θ(z - (-a - ε cos(kx))) - θ(z - (-a))], where a represents height and ε is a small perturbation. The user inquires about the applicability of Green's function technique for solving this equation and whether it can be simplified to a Helmholtz equation. The discussion suggests that simplifying the problem may lead to a superposed solution.

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omyojj
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Hi,
While considering perturbed gravitational potential of incompressible fluid in rectangular configuration, I encountered two dimensional Poisson's equation including the step function.
I want to solve this equation

[tex]\left( \frac{\partial^2}{\partial x^2} + \frac{\partial^2}{\partial z^2} \right) \psi(x, z) = [ \theta( z - ( a + \epsilon \cos(kx) ) } ) - \theta( z - a ) ] + [ \theta( z - ( - a - \epsilon \cos(kx) ) ) - \theta( z - (- a) ) ][/tex]

[tex]a[/tex] is the height from [tex]z=0[/tex] plane and [tex]\epsilon[/tex] is a small number much smaller than [tex]a[/tex].
The source term is periodic in x direction with wavenumber [tex]k[/tex] and has a reflection symmetry.
Hence I expect [tex]\psi[/tex] would be also periodic in x-direction and be an even function about z=0 plane.

Do I have to use green's technique here to solve Poisson's equation involving periodic load?
Can it be reduced to Helmholtz equation in one dimension like [tex]\psi^{\prime \prime} - k^2 \psi = ...[/tex] ?

Any help would be greatly appreciated.

Thank you~
 
Last edited:
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Ok..
What if I simplify the problem?

[tex]\left( \frac{\partial^2}{\partial x^2} + \frac{\partial^2}{\partial z^2} \right) \psi(x, z) = \theta(z - ( a + \epsilon \cos(kx) ) }[/tex]

If I can solve the above one then the superposed solution can be obtained.

help me. T.T
 

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