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Question #43103

Difficulty: 8/10 | 🟢 Free

The Question

An electromagnetic wave propagates in the +x+x direction through a non-magnetic inhomogeneous dielectric medium (μ=μ0\mu = \mu_0). The medium has a spatially varying permittivity ϵ(x)\epsilon(x). At a specific instant t=0t=0, the electric and magnetic fields of the wave are given by: E(x,0)=E0e−αxcos⁡(kx)j^\mathbf{E}(x,0) = E_0 e^{-\alpha x} \cos(kx) \hat{j} B(x,0)=B0e−αxcos⁡(kx)k^\mathbf{B}(x,0) = B_0 e^{-\alpha x} \cos(kx) \hat{k} where E0,B0,α,E_0, B_0, \alpha, and kk are positive constants with appropriate SI units. Calculate the instantaneous rate of change of the total electromagnetic energy density, ∂u∂t\frac{\partial u}{\partial t}, at the position x=π4kx = \frac{\pi}{4k} at t=0t=0.

Options

  • A.

    E0B0μ0e−πα2k(α+k)\frac{E_0 B_0}{\mu_0} e^{-\frac{\pi \alpha}{2k}} (\alpha + k)

  • B.

    2E0B0μ0e−πα2k(α+k)\frac{2 E_0 B_0}{\mu_0} e^{-\frac{\pi \alpha}{2k}} (\alpha + k)

  • C.

    E0B0μ0e−πα2kα\frac{E_0 B_0}{\mu_0} e^{-\frac{\pi \alpha}{2k}} \alpha

  • D.

    E0B0μ0e−πα2kk\frac{E_0 B_0}{\mu_0} e^{-\frac{\pi \alpha}{2k}} k

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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

Poynting Vector and Intensity|Energy Density Locality|Dielectric Polarization Logic|Vector Cross-Product

Why This Question Is Tricky

Common Mistakes

This question tests the student's ability to recognize and apply Poynting's Theorem as a universal conservation law, bypassing missing constitutive data.

The primary trap is the illusion of missing information: students often attempt to calculate energy density using u=12ϵE2+12μ0B2u = \frac{1}{2}\epsilon E^2 + \frac{1}{2\mu_0}B^2, but get stuck because the spatially varying permittivity ϵ(x)\epsilon(x) is deliberately omitted.

A secondary trap lies in the differentiation of the Poynting vector; students accustomed to uniform plane waves may ignore the spatial attenuation factor α\alpha or fail to apply the product rule correctly, leading to incorrect options C or D.

The problem forces the abandonment of steady-state uniform intensity assumptions and demands rigorous application of local differential energy conservation.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterElectromagnetic Waves - Class 12
ConceptPoynting Vector and Intensity
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree