Start Learning Free

Before You Begin

Question #42675

Difficulty: 8/10 | 🟢 Free

The Question

An isolated, uncharged solid conducting sphere of radius RR is placed with its center at the origin (0,0,0)(0,0,0). Two point charges, q1=+2Qq_1 = +2Q and q2=+Qq_2 = +Q, are initially fixed at positions (−d,0,0)(-d, 0, 0) and (d,0,0)(d, 0, 0) respectively, where d≫Rd \gg R. The charge q2q_2 is then displaced by a small distance δ\delta (δ≪d\delta \ll d) along the positive x-axis to a new position (d+δ,0,0)(d+\delta, 0, 0), while q1q_1 remains fixed. What is the new electrostatic potential at a point PP located inside the conducting sphere at (R/2,0,0)(R/2, 0, 0)? (Assume all given variables are in SI units and ϵ0\epsilon_0 is the permittivity of free space).

Options

  • A.

    Q4πϵ0d(3−δd)\frac{Q}{4\pi\epsilon_0 d} \left( 3 - \frac{\delta}{d} \right)

  • B.

    Q4πϵ0d(3−δd−R2d)\frac{Q}{4\pi\epsilon_0 d} \left( 3 - \frac{\delta}{d} - \frac{R}{2d} \right)

  • C.

    Q4πϵ0d(3+δd)\frac{Q}{4\pi\epsilon_0 d} \left( 3 + \frac{\delta}{d} \right)

  • D.

    Q4πϵ0d(3−δd+R2d)\frac{Q}{4\pi\epsilon_0 d} \left( 3 - \frac{\delta}{d} + \frac{R}{2d} \right)

Check Your Answer

Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Variable_Constraint

Develop pure symbolic logic skills by mastering algebraic constraints without relying on numerical data.

Concepts Behind This Question

Conductor Interior Potential|Neutral Equilibrium Points|Approximations (Binomial)

Why This Question Is Tricky

Common Mistakes

This question tests the 'Equipotential Fallacy' in the context of conductors and the superposition principle.

Students often incorrectly assume that the potential at a specific point inside a conductor can be found by simply calculating the potential due to external charges at that exact coordinate, ignoring the crucial role of induced surface charges.

By asking for the potential at an off-center point P(R/2,0,0)P(R/2, 0, 0), the trap lures students into calculating Vext(R/2)V_{ext}(R/2), which yields an incorrect extra term −R2d-\frac{R}{2d} (Option B).

The correct physical framework requires recognizing that the conductor is an equipotential volume, meaning the potential everywhere inside equals the potential at the center.

At the center, the symmetric distance to all induced charges ensures their net potential contribution is zero, allowing the total potential to be calculated solely from the external charges.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterElectrostatic Potential and Capacitance - Class 12
ConceptConductor Interior Potential
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree