What is the Correct Green's Function for a Spherical Shell?

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SUMMARY

The correct Green's function for a hollow spherical shell of radius a is crucial for calculating the potential both inside and outside the sphere. The potential at an arbitrary point is expressed as \(\Phi(r, \theta, \phi)=\frac{1}{4 \pi} \oint \Phi(a, \theta ', \phi ') \frac{\delta G(r, r')}{\delta n '}dS'\), where the Green's function \(G(r, r')\) is defined as \(\frac{1}{(r^2+a^2-2ar\cos \gamma)^{3/2}}-\frac{a}{r'(r^2+\frac{a^4}{r'^2}-2r\frac{a^2}{r'}\cos \gamma)^{3/2}}\). A common error arises in the derivative of the Green's function, where it should be noted that the powers in the denominator must be correctly defined to ensure the potential equals \(V_0\) on the surface of the sphere.

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  • Understanding of Green's functions in electrostatics
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  • Experience with boundary value problems in physics
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kreil
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Homework Statement


If a hollow spherical shell of radius a is held at potential \Phi(a, \theta ', \phi '), then the potential at an arbitrary point is given by,

\Phi(r, \theta, \phi)=\frac{1}{4 \pi} \oint \Phi(a, \theta ', \phi ') \frac{\delta G(r, r')}{\delta n '}dS'

where G(r, r')=\frac{1}{(r^2+a^2-2arcos \gamma)^{3/2}}-\frac{a}{r'(r^2+\frac{a^4}{r'^2}-2r\frac{a^2}{r'}cos \gamma)^{3/2}}

and dS'=a^2 sin(\theta ') d \theta ' d \phi '

Suppose the sphere is held at a fixed potential, V_0.
(a) Calculate the potential outside the sphere.
(b) Use the formula above to calculate the potential inside the sphere.

The Attempt at a Solution



\Phi(r, \theta, \phi)=\frac{V_0}{4 \pi} \oint \frac{\delta G(r, r')}{\delta n '}dS'=\frac{V_0 a^2}{4 \pi}\int_0^{2 \pi} d \phi ' \int_0^{\pi}\frac{\delta G(r, r')}{\delta n '} sin(\theta ') d \theta '=\frac{V_0 a^2}{2}\int_0^{\pi}\frac{\delta G(r, r')}{\delta n '} sin(\theta ') d \theta '
The problem I am having is that when I calculate the potential outside the sphere then set r=a, I do NOT get the potential as being V_0 on the surface as I should.
One spot where I may have messed up is in calculating the derivative of the Green function,

\frac{\delta G(r, r')}{\delta n'}=-\frac{\delta G(r, r')}{\delta r'} |_{r'=a}

I believe this is correct since the normal component of the large sphere points inward along r'..anyway after some algebra I get the answer to be

\frac{2a^2-r^2-racos \gamma}{a(r^2+a^2-2racos \gamma)^{5/2}}

I am thinking either I took this derivative wrong, or I later integrated the expression wrong.

Thanks for your comments.
 
Last edited:
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Hi kreil,

I am pretty sure this is your problem. You have defined your Green function with powers of 3/2 in your denominators when they should rather be powers of 1/2.

I am assuming you have G defined such that on the surface of the sphere, G=0. Well, to prove to yourself which form is correct, try plugging R into x to see which power (1/2 or 3/2) gives you G(x=R)=0.

Good Luck!
 

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