Start Learning Free

Before You Begin

Question #42969

Difficulty: 8/10 | 🟢 Free

The Question

A very long dielectric slab of thickness dd (in meters) along the yy-axis and relative permittivity ϵr\epsilon_r (dimensionless) is moving with a constant velocity v⃗=v0i^\vec{v} = v_0 \hat{i} (in m/s) along its length (the xx-axis). The slab is infinite in the zz-direction. It passes through a region of uniform external magnetic field B⃗ext=B0k^\vec{B}_{ext} = B_0 \hat{k} (in Tesla). Assume v0≪cv_0 \ll c, where cc (in m/s) is the speed of light in vacuum. Due to the motion of the polarized dielectric, an induced magnetic field B⃗ind\vec{B}_{ind} is generated inside the slab. What is the magnitude and direction of B⃗ind\vec{B}_{ind} far from the edges of the slab?

Options

  • A.

    v02c2(ϵr−1)B0k^\frac{v_0^2}{c^2} (\epsilon_r - 1) B_0 \hat{k}

  • B.

    −v02c2(ϵr−1)B0k^-\frac{v_0^2}{c^2} (\epsilon_r - 1) B_0 \hat{k}

  • C.

    v02c2ϵrB0k^\frac{v_0^2}{c^2} \epsilon_r B_0 \hat{k}

  • D.

    −v02c2ϵrB0k^-\frac{v_0^2}{c^2} \epsilon_r B_0 \hat{k}

Check Your Answer

Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Intuition_Breaker

Train your brain to resist "obvious" answers that are designed to deceive your intuition.

Concepts Behind This Question

Magnetic Flux Scalar Sign|Non-Uniform Dielectric Filling|Electric Field Symmetry

Why This Question Is Tricky

Common Mistakes

Students often misapply Lenz's Law, assuming that any induced magnetic field must oppose the external magnetic field, leading them to incorrectly choose the negative sign (Option B).

Furthermore, they frequently confuse the total permittivity with the electric susceptibility, mistakenly using ϵr\epsilon_r instead of (ϵr−1)(\epsilon_r - 1) to calculate the polarization (Option C or D).

The core physical trap lies in failing to recognize that the moving bound charges constitute a polarization current that generates an effective magnetization M⃗=P⃗×v⃗\vec{M} = \vec{P} \times \vec{v}.

Because the polarization P⃗\vec{P} is induced by the motional EMF (v⃗×B⃗\vec{v} \times \vec{B}), the resulting cross-product yields an induced magnetic field that actually enhances the external field, a counter-intuitive result that rigorously tests the integral form of the Maxwell-Ampere law and relativistic field transformations.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterElectromagnetic Induction - Class 12
ConceptMagnetic Flux Scalar Sign
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree