How Does a Dipole Inside a Conducting Shell Affect the Electric Field?

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Homework Help Overview

The discussion revolves around the effects of a dipole placed at the center of a conducting spherical shell within a uniform electric field. Participants are exploring how this configuration influences the electric potential and field, particularly in spherical coordinates.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the potential inside and outside the spherical shell, considering boundary conditions and the behavior of the electric field. There is mention of using the method of image charges and the implications of the dipole's presence on the potential terms.

Discussion Status

The discussion is ongoing, with participants sharing their attempts to apply relevant equations and boundary conditions. Some guidance has been offered regarding the potential terms and the behavior of the electric field inside the shell, but there is no explicit consensus on the correct approach or solution yet.

Contextual Notes

Participants are navigating the complexities of boundary conditions and the implications of the dipole's presence, including considerations of the potential being zero on the spherical shell and the effects of a dielectric material, which introduces additional uncertainty.

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Homework Statement


There is a uniform electric field with strength E_0.Then we place a conducting spherical shell with a dipole at the center of it,inside the field,somehow that the dipole moment is prependicular to the initial field.Find the potential/electric field of the new configuration.(It should be solved in spherical coordinates (r,\theta,\phi) and the answer is independent of \phi.)


Homework Equations



\phi(r,\theta)=\Sigma _{l=0} ^∞ (A_l r^l+\frac{B_l}{r^{l+1}})P_l(cos \theta)
Where A_l and B_l are constants to be determined and P_l(x) are the legendre polynomials.
I'm not sure,but maybe it can be solved by the method of image charges too.

The Attempt at a Solution



I tried to use the formula above but I got so confused about the boundary conditions and also how to use them to calculate As and Bs.
 
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A good start is to look at the potential inside and outside the sphere. On the outside, for example, you can look at r>>R, and on the inside you know that the only thing allowed to blow up is the dipole.
 
Thanks
I tried that,but I thought r>>R means r \rightarrow \infty because otherwise it wouldn't help much.We know that the potential at infinity is -E_0 r cos\theta + A_0 and so I got A_1=-E_0 and A_{l>1}=0.
Then we know that the spherical shell is an equipotential and we can assume it to be zero.
From here,I calculated Bs from l=0 to l=2,using the orthogonality formula for legendre polynomials.They were zero so I suspect all Bs are zero(is it right?). But this means that the potential function is just -E_0 r cos\theta + A_0,which obviously is not.
What have I done wrong?

Can we say that inside the shell,the uniform field is canceled by the rearrangement of charges on the sphere and the only field inside is the field of dipole?

Sorry,I know it makes the problem really different,but what if the sphere was dielectric?

Thanks
 
Last edited:
Not quite, what is the potential term of a dipole? Is there a B_l that will match that term? Hmm, I honestly kind of forget how these problems work with dielectrics.
 
I guess the presence of dipole only changes the boundary conditions which are used to determine the constants and there doesn't need to be sth we call the term associated to the dipole.

Thanks
 

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