Solving a partial differential equation (Helmholtz equation)

Repetit
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Hey!

I am trying to solve this quite nasty (as least I think so : - ) partial differential equation (the Helmholtz equation):

<br /> \frac{1}{r}\frac{\partial}{\partial r} \left( r \frac{\partial\Psi}{\partial r}\right) + \frac{1}{r^2}\frac{\partial^2 \Psi}{\partial \phi^2} + \frac{\partial^2 \Psi}{\partial z^2} + m^2 k^2 \Psi = 0<br />

I use separation of variables and write the unkown function \Psi(r,\phi,z) as \Psi(r,\phi,z) = R(r)\Phi(\phi)Z(z), insert this in the equation and divide by R(r)\Phi(\phi)Z(z). This gives me:

<br /> \frac{1}{r R} \frac{d}{d r} \left( r \frac{d R}{d r}\right) + \frac{1}{r^2 \Phi} \frac{d^2 <br /> \Phi}{d \phi^2} + \frac{1}{Z}\frac{d^2 Z}{d z^2} + m^2 k^2 = 0<br />

Now, I am not sure how to move on from here because I have 1/r^2 in the \Phi term so that I cannot use the usual procedures for solving PDE (equating one term to minus the other terms and setting both equal to some constant). Could someone give me a hint on how to proceed from here?

Thanks in advance
 
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Do two separations. You have
\frac{1}{r R} \frac{d}{d r} \left( r \frac{d R}{d r}\right) + \frac{1}{r^2 \Phi} \frac{d^2 \Phi}{d \phi^2}= \alpha
and
\frac{1}{Z}\frac{d^2 Z}{d z^2} + m^2 k^2 =-\alpha

Now multiply that first equation by r2 to get
\frac{r}{ R} \frac{d}{d r} \left( r \frac{d R}{d r}\right) + \frac{1}{ \Phi} \frac{d^2 \Phi}{d \phi^2} = r^2\alpha
or
\frac{r}{ R} \frac{d}{d r} \left( r \frac{d R}{d r}\right) - r^2\alpha+ \frac{1}{ \Phi} \frac{d^2 \Phi}{d \phi^2} = 0
so that
\frac{r}{ R} \frac{d}{d r} \left( r \frac{d R}{d r}\right) - r^2\alpha= \beta
and
\frac{1}{ \Phi} \frac{d^2 \Phi}{d \phi^2} = -\beta
 
Perfect, thanks a lot! :)
 
Repetit said:
Perfect, thanks a lot! :)
Of course, now you have to know how to solve the radial equation :wink:
 
J77 said:
Of course, now you have to know how to solve the radial equation :wink:

Yes that true :) But the radial equation can be rewritten quite easily into Bessels differential equation.
 
What if k was not a constant but a function of r and z? How does one proceed now?
 
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where Ψ = Stream Function
Δ = ∇^2 (laplacian Operator)
 
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