Potential at a point $x$-distance from the centre inside the conducting sphere of radius $R$ and charged with charge $Q$ is
A$\frac{Q}{R}$
B$\frac{Q}{x}$
C$\frac{Q}{{{x^2}}}$
D$xQ$
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A$\frac{Q}{R}$
a (a) Potential at any point inside the charged spherical conductor equals to the potential at the surface of the conductor i.e. $Q/R$.
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