Conducting Spherical Shell Capacitor

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SUMMARY

The discussion focuses on solving the potential function Φ for a conducting spherical shell divided into upper and lower halves, with the top half at 10V and the bottom half at -10V. The relevant equations include Laplace's equation, expressed in spherical coordinates, and the general solution for Φ involves spherical harmonics. The participant identifies that all B coefficients must be zero to maintain a finite potential at the origin and seeks guidance on applying boundary conditions at radius a. The solution requires expressing the coefficients in integral form to satisfy the specified voltage conditions.

PREREQUISITES
  • Understanding of Laplace's equation in electrostatics
  • Familiarity with spherical coordinates and spherical harmonics
  • Knowledge of boundary value problems in electrostatics
  • Ability to manipulate series expansions and integral forms
NEXT STEPS
  • Study the derivation of spherical harmonics and their applications in electrostatics
  • Learn about boundary value problems and techniques for solving them
  • Explore the method of separation of variables in spherical coordinates
  • Investigate integral representations of coefficients in series expansions
USEFUL FOR

This discussion is beneficial for undergraduate physics students, particularly those studying electromagnetism, as well as educators and anyone interested in advanced electrostatics problems involving spherical geometries.

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Homework Statement


A conducting spherical shell is divided into upper and lower halves with a narrow insulating ring between them. The top half is at 10V and the bottom half is at -10V. Write down the appropriate expansion for Φ and use symmetry and the expected behavior at the origin to identify which coefficients are zero. Then solve for the nonzero coefficients which make Φ satisfy the values given at r = a. You will undoubtedly have to express the coefficients in integral form.


Homework Equations


No charge inside, so Laplace's equation applies:
\nabla^{2}\phi=0
Given the general solution for solving Laplaces equation in spherical coordinates:
\phi (r,\theta,\varphi)= \sum^{\infty}_{n=0}(A_{n}r^{n}+\frac{B^{n}}{r^{n+1}})P_{n}(cos\theta)

The Attempt at a Solution


I've only concluded so far that the B coefficients must all be 0 due to requiring finite potential at r=0. Past that I'm at a loss on how to tackle the function. I know:
\phi (r,\theta,\varphi)= \sum^{\infty}_{n=0}A_{n}r^{n}P_{n}(cos\theta)
But I don't know how I can tackle the boundary condition of plus and minus 10 at radius a, depending on angle theta.

Thanks in advance.
 
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Also I'm not quite sure which forum to put this in. It's a fourth year undergrad course, but all I've been told about the professor is that he gives us grad school type problems like this one, as previous graduates have come back and told us that their graduate EM course was actually easier.
 

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