Can Poisson's Equation Be Solved Using a Legendre Polynomial?

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SUMMARY

The discussion centers on solving Poisson's equation for a positive charge under Debye shielding, specifically the equation \(\nabla^2 \psi = \frac{2}{\lambda^2} \psi\). The correct form of the equation is identified as a Helmholtz equation, not Poisson's. The solution is expressed as \(\psi = \frac{Q}{4\pi\epsilon r} \exp\left(-2 \sqrt{r}/\lambda\right)\). Participants suggest using series solutions and recursion relations to derive coefficients for the solution, emphasizing the importance of correctly identifying the equation type.

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H_man
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Hello,

I have a problem seeing how a solution is reached??

The expression is poisson's equation for a positive charge which is debye shielded.

\nabla . \psi = (2 / \lambda^2) \psi

The solution of which is..

<br /> \psi = (Q / 4\pi\epsilon r )* exp(-2 \sqrt{r}/\lambda) <br />

I was hoping I could express this as a Legendre polynomial but alas, this is only for Laplace's equation it seems.

How can I arrive at this solution?

Thanks,

Harry
 
Last edited:
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Does \psi depend upon \theta and \varphi ?
 
No \theta or \varphi dependence.
 
Then the Poisson's eq becomes a second order ODE. Which can be solved.
 
Oh :blushing: , yeah, I see that now...

Cheers!

Harry
 
What am I missing here...

The first equation expands out to...

V'' + (2/r)V' - (2/c)V = 0

Where I have replaced psi with V.

My standard repository of all mathematical knowledge (Mary L Boas. Mathematical Methods in the Physical Sciences) only covers ODEs which have constant coefficients.

I'm sure there must be a standard technique out there...
 
Well, first thing's first, you have the wrong equation. You have "divergence of scalar equals scalar".

As for your resulting ODE, expand \phi = \sum_j a_j r^j. That should get you a nice recursion relation for the coefficients, and then you're golden.
 
Last edited:
As StatMechGuy said, the equation given isn't Poisson (Laplacian of a function equals something that can only depend on position and time)... and it's weird since a scalar function doesn't have a divergence (did you mean gradient?).
 
First of all

\nabla^2 \psi(r)=\frac{2}{\lambda^2}\psi(r)

is not Poisson equation, but a Helmholtz equation.

It can be written

\frac{1}{r}\frac{d^2}{dr^2}\left[r\psi(r)\right]=\frac{2}{\lambda^2}\psi(r)

\frac{d^2}{dr^2}\left[r\psi(r)\right]=\frac{2}{\lambda^2}\left[r\psi(r)\right]

Can you solve it now ?
 
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Ok I got it (said I... after a little delay).

Thanks Dextercioby, StatMechGuy and Ahmes, I think that's the first time I've used a series solution in anger.

Oh and yes... I initially wrote the equation down incorrectly.. well done to those who spotted it (sorry).
 

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