Potential inside NON-Conducting hollow spherical shell

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SUMMARY

The discussion centers on determining the constants a and b in the potential equation for a non-conducting hollow spherical shell with surface charge density σ and radius R. The potential inside the shell is expressed as V_(x,y,z) = (V0/R²)(6z² + ax² + by²). The solution involves recognizing that the potential is axially symmetric, leading to the conclusion that a and b must equal -3, derived from the Legendre polynomial P₂(cosθ). The Laplacian of the potential relates to the charge density, confirming that the angular distribution must adhere to the properties of spherical harmonics.

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dikmikkel
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Hi Guys,
Suppose we have a spherical shell with charge density on the surface \sigma and radius R. The potential inside the shell is given by:

V_(x,y,z) = \frac{V0}{R^{2}}(6z^2+ax^2+by^2)
It is assumed, that the potential is rotational symmetric around the z-axis inside and outside the shell, and goes to 0 far away from the shell. There's no charge inside and outside the shell and no outer field.

How do i determine the constants a and b?

Mabye change to spherical coordinates and solve the equation:
\frac{\partial{V}}{\partial{\theta}}=0
for a or b. But i can't figure out any other conditions if this is right.
 
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The Laplacian of the voltage is related to the charge. So your boundary conditions would be:

\nabla^2 V = -\frac{\sigma}{\epsilon}

On the surface of the shell. So for ease of analysis you would want to do this in spherical coordinates.
 
I can't really see that this is a boundary condition? And would solving possions equation on the surface help me determine a and b, i can't really follow?
 
Aah sorry I am really tired now. I take the laplacian, and this would relate it all, beautiful, Thanks. Just so used to try finding the potential :)
And sorry for the language. I'm from Denmark.
 
If the pot inside is axially symjmetric, and b must be equal.
Since DEl^2 V=0 inside, the angular distribution must be a Legendre polynomial.
Since the power of x,y,and z is 2, it must be
P_2(\cos\theta)=(3\cos^2\theta-1)/2.
This means a=b=-3.
 
Last edited by a moderator:
That's gold thank you.
 

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