In the previous question assume that the electrostatic potential is zero at an infinite distance from the spherical shell. The electrostatic potential at a distance `R (a lt R lt b)` from the centre of the shell is where `(K=1/(4pi epsilon_(0)))`

Both question (33) and (34) refer to the system of charges as shown in the figure. A spherical shell with an inner radius 'a' and an outer radius 'b' is made of conducting material. A point charge +Q is placed at the centre of the spherical shell and a total charge -q is placed on the shell. Assume that the electrostatic potential is zero at an infinite distance from the spherical shell. The electrostatic potential at a distance R(a lt R lt b) from the centre of the shell is

Electric potential due to a dipole at a position vec r from its centre is: where (K = 1/(4pi epsilon_0)

Electric potential due to a dipole at a position vec r from its centre is: where (K = 1/(4pi epsilon_0)

The electrostatic potential of a uniformly charged thin spherical shell of charge Q and radius R at a distance r from the centre

The electrostatic potential of a uniformly charged thin spherical shell of charge Q and radius R at a distance r from the centre

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 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 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