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Question #42982

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The Question

A large rectangular dielectric slab of thickness dd (spanning from y=0y=0 to y=dy=d) moves with a constant velocity v⃗=v0i^\vec{v} = v_0 \hat{i} through a uniform, time-independent magnetic field B⃗=B0k^\vec{B} = B_0 \hat{k}. The relative permittivity of the dielectric material varies non-uniformly along the yy-axis as ϵr(y)=K0ey/d\epsilon_r(y) = K_0 e^{y/d}, where K0>1K_0 > 1 is a constant. Assuming there are no free charges present anywhere and the magnetic Reynolds number is negligibly small, what is the magnitude of the steady-state potential difference ΔV\Delta V between the surfaces y=0y=0 and y=dy=d in the laboratory frame?

Options

  • A.

    v0B0d(1−e−1K0e)v_0 B_0 d \left( 1 - \frac{e-1}{K_0 e} \right)

  • B.

    v0B0d(e−1K0e)v_0 B_0 d \left( \frac{e-1}{K_0 e} \right)

  • C.

    v0B0dv_0 B_0 d

  • D.

    v0B0d(1−1K0e)v_0 B_0 d \left( 1 - \frac{1}{K_0 e} \right)

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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

Motional EMF for Arbitrary Shapes|Electric Field Symmetry|Non-Uniform Dielectric Filling

Why This Question Is Tricky

Common Mistakes

This question tests the synthesis of motional induction and electrostatics in non-uniform dielectrics.

A common trap is for students to incorrectly assume that the dielectric simply attenuates the motional EMF by a factor of ϵr\epsilon_r, leading to E=vB/ϵrE = vB/\epsilon_r (Option B).

This misapplies the concept of dielectric shielding, which is valid for external fields but not for internal motional EMFs.

The correct physical framework requires applying Gauss's Law for the displacement field (∇⋅D⃗=0\nabla \cdot \vec{D} = 0).

Because the polarization is driven by the Lorentz force in the moving frame (E⃗′=E⃗+v⃗×B⃗\vec{E}' = \vec{E} + \vec{v} \times \vec{B}), the boundary condition Dy=0D_y = 0 dictates that the internal electric field is Ey=vB(1−1/ϵr)E_y = vB(1 - 1/\epsilon_r).

Ignoring the depolarizing effect of the bound charges induced by the motional EMF leads to fundamental errors in calculating the potential difference.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterElectromagnetic Induction - Class 12
ConceptMotional EMF for Arbitrary Shapes
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree