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| 1. |
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 isA. `(2Q)/(4piepsilon_(0)R)`B. `(2Q)/(4piepsilon_(0)R)-(2q)/(4piepsilon_(0)R)`C. `(2Q)/(4piepsilon_(0)R)+(2q)/(4piepsilon_(0)R)`D. `((q+Q))/(4piepsilon_(0))(2)/(R)` |
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