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A thin spherical conducting shell of radius R has a charge q. Another charge Q is placed at the centre of the shell. The electrostatic potential at a point P at a distance R/2 from the centre of the shell is :


( A ) (q+Q)4πε02R
( B ) 2Q4πε0R2q4πε0R
( C ) 2Q4πε0R+q4πε0R
( D ) 2Q4πε0R

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