Potential of a dipole with actual physical extension?

AI Thread Summary
The discussion explores the potential of a dipole with physical extension, specifically a metal sphere with radius R and a defined dipole moment. It highlights that if the surface charge distribution varies as cos theta, the external field resembles that of an ideal dipole located at the sphere's center. Additionally, it notes that the electric field inside the sphere remains constant. The use of Coulomb's law is suggested for calculating the actual field configuration. Overall, the conversation emphasizes the relationship between surface charge distribution and dipole potential.
Gavroy
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I think everybody here knows the equation that gives the potential of a point like dipole, but how does the field look like if you have e.g. a metal sphere with radius $R$ and a certain dipol moment, how does this potential look like?
 
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If the surface charge varies like cos theta, the field outside will equal to that of an ideal dipole in the center of the sphere. Inside the sphere, the field is constant. Using Coulombs law it is easy to work out the actual field configuration.
 
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