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Question
For a uniformly charged thin spherical shell, what is the electric field at any point inside the shell (r < R)?
Options
\[E = \frac{1}{4\pi\varepsilon_0} \cdot \frac{Q}{R^2}\]
\[E = \frac{Q}{4\pi\varepsilon_0 R}\]
\[E = \frac{Q}{4\pi\varepsilon_0 r^2}\]
E = 0
MCQ
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Solution
Inside a uniformly charged spherical shell, the electric field is zero everywhere. This is a fundamental result derived from Gauss's Law: when a concentric Gaussian surface is drawn inside the shell (r < R), it encloses zero charge, so the flux through it is zero and therefore E = 0. This is a key property of spherical shells.
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