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Electrostatics question

2003 · Shift 0 · Q168
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Electrostatics question

2003 · Shift 0 · Q168

JEE MainPhysicsElectrostaticsMCQ+4 / −1
A thin spherical conducting shell of radius RRR has a charge q.q.q. Another charge QQQ is placed at the center of the shell. The electrostatic potential at a point PPP a distance R2{R \over 2}2R​ from the center of the shell is
  1. A
    2Q4πε0R{{2Q} \over {4\pi {\varepsilon _0}R}}4πε0​R2Q​
  2. B
    2Q4πε0R−2q4πε0R{{2Q} \over {4\pi {\varepsilon _0}R}} - {{2q} \over {4\pi {\varepsilon _0}R}}4πε0​R2Q​−4πε0​R2q​
  3. C
    2Q4πε0R+q4πε0R{{2Q} \over {4\pi {\varepsilon _0}R}} + {q \over {4\pi {\varepsilon _0}R}}4πε0​R2Q​+4πε0​Rq​
  4. D
    (q+Q)24πε0R{{\left( {q + Q} \right)2} \over {4\pi {\varepsilon _0}R}}4πε0​R(q+Q)2​
View written solutionFree

Correct answer: C

  1. Understand the charge distribution on the conducting shell

A conducting spherical shell of radius RRR has net charge qqq. A point charge QQQ is placed at the center.

Because of electrostatic induction:

  • charge induced on the inner surface =−Q= -Q=−Q
  • charge induced on the outer surface =q+Q= q+Q=q+Q

This is because the total charge on the conductor must remain qqq.


  1. Find potential at point PPP inside the shell

Point PPP is at distance R/2R/2R/2 from the center, so it lies inside the shell.

Potential at PPP is the algebraic sum of potentials due to:

  • central charge QQQ
  • inner spherical surface charge −Q-Q−Q
  • outer spherical surface charge q+Qq+Qq+Q

  1. Potential due to central charge QQQ at r=R/2r=R/2r=R/2

V1=14πε0QR/2=2Q4πε0RV_1 = \frac{1}{4\pi\varepsilon_0}\frac{Q}{R/2} = \frac{2Q}{4\pi\varepsilon_0 R}V1​=4πε0​1​R/2Q​=4πε0​R2Q​


  1. Potential due to inner surface charge −Q-Q−Q

The inner surface is a spherical shell of radius RRR. For any point inside a uniformly charged spherical shell, potential is constant and equal to the surface potential:

V2=14πε0−QRV_2 = \frac{1}{4\pi\varepsilon_0}\frac{-Q}{R}V2​=4πε0​1​R−Q​


  1. Potential due to outer surface charge q+Qq+Qq+Q

Similarly, for the outer spherical shell:

V3=14πε0q+QRV_3 = \frac{1}{4\pi\varepsilon_0}\frac{q+Q}{R}V3​=4πε0​1​Rq+Q​


  1. Add all contributions

VP=V1+V2+V3V_P = V_1 + V_2 + V_3VP​=V1​+V2​+V3​

VP=2Q4πε0R+−Q4πε0R+q+Q4πε0RV_P = \frac{2Q}{4\pi\varepsilon_0 R} + \frac{-Q}{4\pi\varepsilon_0 R} + \frac{q+Q}{4\pi\varepsilon_0 R}VP​=4πε0​R2Q​+4πε0​R−Q​+4πε0​Rq+Q​

VP=2Q−Q+q+Q4πε0RV_P = \frac{2Q - Q + q + Q}{4\pi\varepsilon_0 R}VP​=4πε0​R2Q−Q+q+Q​

VP=2Q+q4πε0RV_P = \frac{2Q+q}{4\pi\varepsilon_0 R}VP​=4πε0​R2Q+q​

So,

VP=2Q4πε0R+q4πε0RV_P = \frac{2Q}{4\pi\varepsilon_0 R} + \frac{q}{4\pi\varepsilon_0 R}VP​=4πε0​R2Q​+4πε0​Rq​


  1. Match with options

This matches Option C.


  1. Comparison with stored correct answer

Stored correct answer: C

Derived answer: C

So they agree.

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