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Question: A point charge \( q \) is a distance \( r \) from the centre O of an uncharged conducting layer whos...

A point charge qq is a distance rr from the centre O of an uncharged conducting layer whose inner and outer radii equal to aa and bb respectively. The potential at the point O if a<ra < r is q4πε0\dfrac{q}{{4\pi {\varepsilon _0}}} times
(A) (1r1a+1b)\left( {\dfrac{1}{r} - \dfrac{1}{a} + \dfrac{1}{b}} \right)
(B) (1a1r+1b)\left( {\dfrac{1}{a} - \dfrac{1}{r} + \dfrac{1}{b}} \right)
(C) (1b1a1r)\left( {\dfrac{1}{b} - \dfrac{1}{a} - \dfrac{1}{r}} \right)
(D) (1a1b1r)\left( {\dfrac{1}{a} - \dfrac{1}{b} - \dfrac{1}{r}} \right)

Explanation

Solution

Hint : Since, the conducting sphere is uncharged the total charge in the sphere is equal to zero. The charge inside the layer will induce a negative charge at the inner layer, and hence induce a positive charge on the outer layer.

Formula used: In this solution we will be using the following formula;
V=q4πε0rV = \dfrac{q}{{4\pi {\varepsilon _0}r}} where VV is the electric potential, qq is the charge creating an electric field, ε0{\varepsilon _0} is the permittivity of free space and rr is the distance of interest from the charge.

Complete step by step answer:
Now, a charge qq was said to be placed inside an uncharged spherical layer at a distance rr away from the centre. Hence, due to the charge qq only at the centre is equal to
V=q4πε0rV = \dfrac{q}{{4\pi {\varepsilon _0}r}}
However, due to the charge, the inner layer will be induced with charge q- q and since the layer is in general uncharged the outer layer will have a charge qq . Hence, the total electric potential will be
Vt=q4πε0r+q4πε0a+q4πε0b{V_t} = \dfrac{q}{{4\pi {\varepsilon _0}r}} + \dfrac{{ - q}}{{4\pi {\varepsilon _0}a}} + \dfrac{q}{{4\pi {\varepsilon _0}b}} where aa is the inner radius of the sphere and bb is the outer radius.
Hence, by factoring out all common quantities and constants, we have
Vt=q4πε0(1r1a+1b){V_t} = \dfrac{q}{{4\pi {\varepsilon _0}}}\left( {\dfrac{1}{r} - \dfrac{1}{a} + \dfrac{1}{b}} \right)
Which means that q4πε0\dfrac{q}{{4\pi {\varepsilon _0}}} multiplies (1r1a+1b)\left( {\dfrac{1}{r} - \dfrac{1}{a} + \dfrac{1}{b}} \right) .
Thus, the correct option is A.

Note:
For clarity, the reason why the inner radius gets a negative charge is because of the attraction of the negative charges in the conducting layer to the positive charge close to the centre. Recall that a conducting layer, although may be generally neutral in charge, contains free electrons. The migration of the negative charge to the inner part of the sphere allows the outer layer to build up positive charges.