Solution:
The electric potential at the surface of a conducting sphere is \(V = \frac{kQ}{R} \implies kQ = VR\). The electric field at any point outside the sphere (\(r > R\)) is \(E = \frac{kQ}{r^2} = \frac{VR}{r^2}\).
The electric potential at the surface of a conducting sphere is \(V = \frac{kQ}{R} \implies kQ = VR\). The electric field at any point outside the sphere (\(r > R\)) is \(E = \frac{kQ}{r^2} = \frac{VR}{r^2}\).
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