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
\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) ) ]
a is the height from z=0 plane and \epsilon is a small number much smaller than a.
The source term is periodic in x direction with wavenumber k and has a reflection symmetry.
Hence I expect \psi 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 \psi^{\prime \prime} - k^2 \psi = ... ?
Any help would be greatly appreciated.
Thank you~
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
\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) ) ]
a is the height from z=0 plane and \epsilon is a small number much smaller than a.
The source term is periodic in x direction with wavenumber k and has a reflection symmetry.
Hence I expect \psi 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 \psi^{\prime \prime} - k^2 \psi = ... ?
Any help would be greatly appreciated.
Thank you~
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