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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 a distance `R/2` from the centre of the shell is
A. `((q+_Q))/(4pi epsilon_(0))(2)/(R)`
B. `(2Q)/(4pi epsilon_(0)R)`
C. `(2Q)/(4 pi epsilon_(0)R)-(2q)/(4pi epsilon_(0)R)`
D. `(2Q)/(4pi epsilon_(0)R)+(q)/(4pi epsilon_(0)R)`

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