(1) An infinite number of point charges each equal to +Q coulomb are arranged at random around a point P such that the distances of the charges from the point P are 1m, 2m, 4m, 8m, 16m,…….etc... The electric potential at P is
(a) zero (b) infinite (c) negligibly small
(d) Q/2πε0 (e) Q/4πε0
Note that the electric potential is a scalar quantity. Therefore, the direction of the location of the charge does not matter and the potentials simply add up. The resultant potential (V) at P is given by
V = (Q/4πε0) × [(1/1) + (1/2) + (1/4) + (1/8) + ………]
The infinite series within the square bracket yields a value equal to 2 so that V = Q/2πε0.
(2) A thin spherical conducting shell of radius R has a charge +Q. Another point charge –q is placed at the centre of the shell. The electrostatic potential at a point P distant R/2 from the centre of the shell is
(a) (Q/4πε0R) – (2q/4πε0R) (b) (q/4πε0R) – (2Q/4πε0R)
(c) – (2q/4πε0R) (d) (Q/4πε0R) (e) zero
The electrostatic potential at any point within the shell due to the charge Q on the shell is constant and is equal to Q/4πε0R.
The potential at distance R/2 due to the charge –q placed at the centre of the shell is – q/4πε0(R/2) = – 2q/4πε0R.
Therefore, the net potential (V) at the point P distant R/2 from the centre of the shell is given by
V = (Q/4πε0R) – (2q/4πε0R), given in option (a).
[Note that positive charges will produce positive potential where as negative charges will produce negative potential].
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