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Question: The capacitance of two concentric spherical shells of radii \( {R_1} \) and \( {R_2} \) \( \left( {{...

The capacitance of two concentric spherical shells of radii R1{R_1} and R2{R_2} (R2>R1)\left( {{R_2} > {R_1}} \right) is:
(A) 4πε0R24\pi {\varepsilon _0}{R_2}
(B) 4πε0R2R1R1R24\pi {\varepsilon _0}\dfrac{{{R_2} - {R_1}}}{{{R_1}{R_2}}}
(C) 4πε0R1R2R2R14\pi {\varepsilon _0}\dfrac{{{R_1}{R_2}}}{{{R_2} - {R_1}}}
(D) 4πε0R14\pi {\varepsilon _0}{R_1}

Explanation

Solution

To solve this question, we need to consider a charge on the system of spherical shells. Then we have to find out the potential difference in the system with the help of the charge distribution in the system. Finally, we have to apply the basic formula of the capacitance to get the final answer.

Formula used: The formulae which are used to solve this question are given by
V=Q4πε0R\Rightarrow V = \dfrac{Q}{{4\pi {\varepsilon _0}R}} , here VV is the potential on a sphere of radius RR which has a charge of QQ.
C=QV\Rightarrow C = \dfrac{Q}{V} , here CC is the capacitance, QQ is the charge, and VV is the potential difference.

Complete step by step answer
Let us consider the two spherical shells of radii R1{R_1} and R2{R_2} as shown in the figure below. Let the outer sphere be charged with a charge of +Q+ Q. The charge will get distributed on the whole surface of the outer spherical shell.

Due to the positive charge on the outer sphere, an equal amount of positive charge will appear at the outer surface of the inner sphere, as shown in the figure below.

So the potential of the outer spherical shell becomes
V1=Q4πε0R2\Rightarrow {V_1} = \dfrac{Q}{{4\pi {\varepsilon _0}{R_2}}} ………………….(1)
Also the potential of the inner spherical shell is
V2=Q4πε0R1\Rightarrow {V_2} = \dfrac{Q}{{4\pi {\varepsilon _0}{R_1}}} ………………………….(2)
So the net potential difference between the two spherical shells is
V=V2V1\Rightarrow V = {V_2} - {V_1}
From (1) and (2)
V=Q4πε0R1Q4πε0R2\Rightarrow V = \dfrac{Q}{{4\pi {\varepsilon _0}{R_1}}} - \dfrac{Q}{{4\pi {\varepsilon _0}{R_2}}}
V=Q4πε0(1R11R2)\Rightarrow V = \dfrac{Q}{{4\pi {\varepsilon _0}}}\left( {\dfrac{1}{{{R_1}}} - \dfrac{1}{{{R_2}}}} \right)
On simplifying we get
V=Q(R2R1)4πε0R1R2\Rightarrow V = \dfrac{{Q\left( {{R_2} - {R_1}} \right)}}{{4\pi {\varepsilon _0}{R_1}{R_2}}} ……………(3)
Now we know that the capacitance is given by
C=QV\Rightarrow C = \dfrac{Q}{V}
Substituting (3) we have
C=QQ(R2R1)4πε0R1R2\Rightarrow C = \dfrac{Q}{{\dfrac{{Q\left( {{R_2} - {R_1}} \right)}}{{4\pi {\varepsilon _0}{R_1}{R_2}}}}}
On simplifying, we finally get
C=4πε0R1R2R2R1\Rightarrow C = 4\pi {\varepsilon _0}\dfrac{{{R_1}{R_2}}}{{{R_2} - {R_1}}}
Thus, the capacitance of the given two concentric spherical shells is equal to 4πε0R1R2R2R14\pi {\varepsilon _0}\dfrac{{{R_1}{R_2}}}{{{R_2} - {R_1}}}.

Hence, the correct answer is option C.

Note
This question could also be attempted by considering the electric field at an arbitrary point between the two spherical shells to find out the net potential difference. Then applying the formula for the capacitance as above will give the final answer.