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

In summary, the formula for calculating the potential at an arbitrary point due to a hollow spherical shell held at a fixed potential is given by \Phi(r, \theta, \phi)=\frac{V_0}{4 \pi} \oint \frac{\delta G(r, r')}{\delta n '}dS', where G(r, r')=\frac{1}{(r^2+a^2-2arcos \gamma)^{1/2}}-\frac{a}{r'(r^2+\frac{a^4}{r'^2}-2r\frac{a^2}{r'}cos \gamma)^{1/2}} and dS'=a^2 sin(\theta ')
  • #1
kreil
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Homework Statement


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

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

where [tex]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}}[/tex]

and [tex]dS'=a^2 sin(\theta ') d \theta ' d \phi '[/tex]

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

The Attempt at a Solution



[tex]\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 '[/tex]
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 [itex]V_0[/itex] on the surface as I should.
One spot where I may have messed up is in calculating the derivative of the Green function,

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

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

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

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

Thanks for your comments.
 
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  • #2
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!
 

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

What is the Green's function for the sphere?

The Green's function for the sphere is a mathematical function used to describe the response of a spherical object to an external force or source. It is commonly used in electromagnetics, acoustics, and other fields of physics and engineering.

How is the Green's function for the sphere derived?

The Green's function for the sphere is derived using boundary value problems and the method of images. This involves solving for the electric or acoustic potential in the presence of a spherical object and then applying boundary conditions to find the Green's function.

What are the applications of the Green's function for the sphere?

The Green's function for the sphere has many practical applications, including calculating the scattering of electromagnetic or acoustic waves off of a spherical object, determining the response of a spherical antenna or microphone, and simulating the behavior of particles in a spherical potential.

What are the limitations of the Green's function for the sphere?

While the Green's function for the sphere is a useful tool for solving certain problems, it is limited to systems with spherical symmetry. This means it cannot be applied to non-spherical objects or systems with complex geometries.

How does the Green's function for the sphere relate to other Green's functions?

The Green's function for the sphere is a special case of the more general Green's function for a point source. It can also be related to the Green's function for a line source in the limit of a very thin sphere. Additionally, the Green's function for the sphere can be used to construct the Green's function for other shapes through superposition and the method of images.

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