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Question
The electric potential on the surface of a uniformly charged spherical shell of radius \[R\] carrying charge \[q\] is:
Options
\[V = \frac{1}{4\pi\varepsilon_0}\frac{q}{R^2}\]
\[V = \frac{1}{4\pi\varepsilon_0}\frac{q}{2R}\]
\[V = \frac{1}{4\pi\varepsilon_0}\frac{q}{R}\]
\[V = 0\]
MCQ
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Solution
On the surface \[(r = R)\], the potential is \[V = \frac{1}{4\pi\varepsilon_0}\frac{q}{R}\]. This value is continuous with both the outside expression (setting \[r = R\]) and the constant interior value, ensuring potential is continuous everywhere.
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