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Question #43366

Difficulty: 8/10 | 🟢 Free

The Question

A parallel plate capacitor has plate area AA and separation dd. The space between the plates is filled with a non-uniform, lossy dielectric. The real permittivity ϵ(x)\epsilon(x) and electrical conductivity σ(x)\sigma(x) of the dielectric vary with the distance xx from one plate (0≤x≤d0 \le x \le d) as: ϵ(x)=ϵ0(1+xd)2,σ(x)=σ0(1+xd)2\epsilon(x) = \epsilon_0 \left(1 + \frac{x}{d}\right)^2, \quad \sigma(x) = \sigma_0 \left(1 + \frac{x}{d}\right)^2 The capacitor is connected to an AC voltage source of angular frequency ω\omega. The source has an internal resistance R0R_0 and an internal inductance L0L_0. To ensure that the maximum possible average power is transferred from the source to the lossy capacitor, what must be the values of R0R_0 and L0L_0? (Assume edge effects are negligible).

Options

  • A.

    R0=σ0d2A(σ02+ω2ϵ02)R_0 = \frac{\sigma_0 d}{2A(\sigma_0^2 + \omega^2 \epsilon_0^2)}, L0=ϵ0d2A(σ02+ω2ϵ02)L_0 = \frac{\epsilon_0 d}{2A(\sigma_0^2 + \omega^2 \epsilon_0^2)}

  • B.

    R0=d2σ0AR_0 = \frac{d}{2\sigma_0 A}, L0=d2ω2ϵ0AL_0 = \frac{d}{2\omega^2 \epsilon_0 A}

  • C.

    R0=3σ0d7A(σ02+ω2ϵ02)R_0 = \frac{3\sigma_0 d}{7A(\sigma_0^2 + \omega^2 \epsilon_0^2)}, L0=3ϵ0d7A(σ02+ω2ϵ02)L_0 = \frac{3\epsilon_0 d}{7A(\sigma_0^2 + \omega^2 \epsilon_0^2)}

  • D.

    R0=σ0dA(σ02+ω2ϵ02)R_0 = \frac{\sigma_0 d}{A(\sigma_0^2 + \omega^2 \epsilon_0^2)}, L0=ϵ0dA(σ02+ω2ϵ02)L_0 = \frac{\epsilon_0 d}{A(\sigma_0^2 + \omega^2 \epsilon_0^2)}

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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

Maximum Power Transfer|Non-Uniform Dielectric Filling|Capacitive Reactance Dependency

Why This Question Is Tricky

Common Mistakes

This question tests the application of the Maximum Power Transfer theorem to complex, distributed impedances.

The primary trap lies in incorrectly modeling the equivalent circuit of the non-uniform lossy dielectric.

Students often calculate the total equivalent series resistance ReqR_{eq} and total equivalent series capacitance CeqC_{eq} independently by integrating dRdR and dC−1dC^{-1}, and then erroneously combine them in series as ZL=Req−j/(ωCeq)Z_L = R_{eq} - j/(\omega C_{eq}) (Option B).

However, physically, the conduction and displacement currents flow in parallel through each infinitesimal slice dxdx, meaning the local resistance and capacitance are in parallel, while the slices themselves are in series.

Furthermore, the problem requires applying the complex conjugate matching condition (ZS=ZL∗Z_S = Z_L^*) rather than merely equating magnitudes, testing a deeper understanding of AC power transfer.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterCurrent Electricity - Class 12
ConceptMaximum Power Transfer
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree