Solving Capacitance Problem: Identical Answers Explained

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The discussion centers on the similarity between two problems involving concentric conducting shells and their capacitance. Both scenarios yield the same capacitance formula despite differing configurations, as the presence of an intermediate conductor does not alter the electric field due to spherical symmetry. The potential remains constant on metal surfaces, and replacing an equipotential surface with a thin metal foil does not affect the electric field. The net charge on the metal shell remains zero, ensuring that induced charges do not change the overall electric field. Understanding these principles clarifies why both setups result in identical capacitance calculations.
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Homework Statement


Why are both these problems identical?
In both cases, c>b>a.
Q1 Three concentric conducting shells A, B and C of radii a, b and c are arranged as shown. A dielectric of dielectric constant K is filled between A and B. Find the capacitance between A and C.

Q2 A spherical capacitor is made of two conducting spherical shells of radii a and c. The space between the shells is filled with a dielectric of dielectric constant K unto a radius b as shown. Find the capacitance of the system.

Homework Equations

The Attempt at a Solution


Both have answers (4πεo.Kabc)/(Ka(c-b)+c(b-a))
I know how to do the first one, but I don't understand why both have the same answer, ie. why the capacitance of the system is equal to the capacitance between A and C.
 
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Assume a charge of Q on the inner conductor. Does the presence of the conductor B change the electric field in the two regions between the two cases?
 
vela said:
Assume a charge of Q on the inner conductor. Does the presence of the conductor B change the electric field in the two regions between the two cases?
I know it doesn't mathematically, but I'm not getting a feel for it.
 
The potential is constant on a metal surface. Because of spherical symmetry, the equipotential surfaces are concentric spheres between A and C.
Replacing an equipotential surface with a very thin metal foil does not change anything, the electric field stays the same. That thin metal shell can be placed at radius b, and nothing is changed, but the set-up becomes identical with the first one.
 
ehild said:
The potential is constant on a metal surface. Because of spherical symmetry, the equipotential surfaces are concentric spheres between A and C.
Replacing an equipotential surface with a very thin metal foil does not change anything, the electric field stays the same. That thin metal shell can be placed at radius b, and nothing is changed, but the set-up becomes identical with the first one.
But won't the metal surface induce charges on it's inner and outer surfaces, and thus alter the electric field?
 
The electric field induce charge on both surfaces of the metal, but the net charge of the shell remains zero.
Well, calculate the electric field below and above the middle metal shell, applying Gauss' Law.
 
Got it! Thanks :)
 
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