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Question #42842

Difficulty: 8/10 | 🟢 Free

The Question

An isolated thin metallic spherical shell of initial radius R0 mR_0 \text{ m} carries a constant total charge Q CQ \text{ C}. The shell is in a vacuum. Initially, the electric field magnitude just outside the surface of the shell is E0 V/mE_0 \text{ V/m} and the total electric flux through a spherical Gaussian surface infinitesimally larger than the shell is Φ0 V⋅m\Phi_0 \text{ V}\cdot\text{m}. The temperature of the shell is then uniformly increased by ΔT K\Delta T \text{ K}. If the coefficient of linear thermal expansion of the shell material is α K−1\alpha \text{ K}^{-1} (where αΔT≪1\alpha \Delta T \ll 1), what are the fractional changes in the electric field magnitude (ΔEE0\frac{\Delta E}{E_0}) just outside the shell and the total electric flux (ΔΦΦ0\frac{\Delta \Phi}{\Phi_0}) through the new infinitesimally larger Gaussian surface, respectively?

Options

  • A.

    −2αΔT-2\alpha \Delta T and 00

  • B.

    00 and 2αΔT2\alpha \Delta T

  • C.

    2αΔT2\alpha \Delta T and 00

  • D.

    −2αΔT-2\alpha \Delta T and 2αΔT2\alpha \Delta T

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Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Multi-Concept_Bridge

Master problems that require linking physics and math concepts to solve complex competitive questions.

Concepts Behind This Question

Flux and Surface Geometry|Thermal Expansion of Area and Volume|Surface Integration

Why This Question Is Tricky

Common Mistakes

This question tests the conceptual distinction between Gauss's Law (which dictates total flux) and the local electric field boundary condition at a conductor's surface.

A common trap for JEE candidates is assuming that because the total enclosed charge and total flux remain constant, the electric field just outside the surface must also remain constant.

However, thermal expansion increases the surface area (A∝R2A \propto R^2), which decreases the surface charge density (σ=Q/A\sigma = Q/A).

Consequently, the local electric field (E=σ/ϵ0E = \sigma/\epsilon_0) decreases by a fractional amount of −2αΔT-2\alpha \Delta T, even though the total flux (Φ=∮E⃗⋅dA⃗\Phi = \oint \vec{E} \cdot d\vec{A}) is perfectly conserved.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterElectric Charges and Fields - Class 12
ConceptFlux and Surface Geometry
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree