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Question #43169

Difficulty: 8/10 | 🟢 Free

The Question

A plane electromagnetic wave with electric field E⃗i=E0cos⁡(ωt−kz)i^\vec{E}_i = E_0 \cos(\omega t - kz) \hat{i} is incident normally on a thin, infinite resistive sheet located at z=0z=0. The sheet has a uniform surface conductivity σs=4μ0c\sigma_s = \frac{4}{\mu_0 c}, such that the induced surface current density is K⃗=σsE⃗sheet\vec{K} = \sigma_s \vec{E}_{sheet}. Here μ0\mu_0 is the vacuum permeability, ϵ0\epsilon_0 is the vacuum permittivity, and cc is the speed of light in vacuum. Determine the time-averaged radiation pressure ⟨P⟩\langle P \rangle exerted on the sheet.

Options

  • A.

    23ϵ0E02\frac{2}{3} \epsilon_0 E_0^2

  • B.

    29ϵ0E02\frac{2}{9} \epsilon_0 E_0^2

  • C.

    12ϵ0E02\frac{1}{2} \epsilon_0 E_0^2

  • D.

    49ϵ0E02\frac{4}{9} \epsilon_0 E_0^2

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

Transverse Nature of EM Waves|Gauss Law Applicability|Symmetry and Virtual Work

Why This Question Is Tricky

Common Mistakes

This question targets a profound misconception regarding radiation pressure on partially absorbing/reflecting boundaries.

Students frequently assume that radiation pressure can be calculated merely by finding the absorbed intensity (Iabs=12σsEt2I_{abs} = \frac{1}{2}\sigma_s E_t^2) and dividing by cc, which incorrectly yields 29ϵ0E02\frac{2}{9}\epsilon_0 E_0^2.

They treat the dynamic wave interaction as a simple inelastic collision, ignoring the momentum carried away by the reflected and transmitted waves.

Furthermore, if attempting a microscopic force analysis, students often incorrectly use the total magnetic field on one side of the sheet rather than the average field B⃗avg\vec{B}_{avg} acting on the surface current, or they mistakenly apply a static Gauss-like gradient F=qEF=qE which averages to zero.

The correct approach requires either rigorous momentum conservation (pin+pref−ptransp_{in} + p_{ref} - p_{trans}) or evaluating the Lorentz force with the correct phase and average B-field.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterElectromagnetic Waves - Class 12
ConceptTransverse Nature of EM Waves
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree