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Question #43599

Difficulty: 8/10 | 🟢 Free

The Question

A rigid square conducting loop of side LL and total resistance RR lies in the xyxy-plane. At t=0t=0, it is pulled with a constant velocity v0i^v_0 \hat{i} into a region x>0x > 0 containing a uniform magnetic field B0k^B_0 \hat{k}. Mounted on the loop is an optical system consisting of a fixed polarizer and a second polarizer rotating at a constant angular velocity ω\omega. Unpolarized light of intensity 2I02I_0 is incident on the system, such that the transmitted intensity is I(t)=I0cos⁡2(ωt)I(t) = I_0 \cos^2(\omega t). A transducer on the loop uses this light to generate an additional uniform magnetic field Bint(t)=βI(t)k^B_{int}(t) = \beta I(t) \hat{k} strictly confined within the entire area L2L^2 of the loop. Neglecting self-inductance, what is the average electrical power dissipated in the loop as heat during the time it is partially inside the external magnetic field? (Assume the time taken to enter is much larger than 2π/ω2\pi/\omega).

Options

  • A.

    B02L2v02R\frac{B_0^2 L^2 v_0^2}{R}

  • B.

    B02L2v02R+β2I02L4ω22R\frac{B_0^2 L^2 v_0^2}{R} + \frac{\beta^2 I_0^2 L^4 \omega^2}{2R}

  • C.

    B02L2v02R+β2I02L4ω2R\frac{B_0^2 L^2 v_0^2}{R} + \frac{\beta^2 I_0^2 L^4 \omega^2}{R}

  • D.

    B02L2v02R+β2I02L4ω24R\frac{B_0^2 L^2 v_0^2}{R} + \frac{\beta^2 I_0^2 L^4 \omega^2}{4R}

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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

Malus's Law|Lenz's Law Energy Conservation|Variable Force Integration

Why This Question Is Tricky

Common Mistakes

This question tests a lethal misconception regarding the Work-Energy Theorem in electrodynamics.

Students often blindly assume that the average electrical power dissipated in a moving loop equals the average mechanical power supplied by the external pulling force (⟨Pmech⟩=⟨Fextv0⟩\langle P_{mech} \rangle = \langle F_{ext} v_0 \rangle).

If they calculate the magnetic drag force Fmag=iLB0F_{mag} = i L B_0, they will find ⟨Pmech⟩=B02L2v02R\langle P_{mech} \rangle = \frac{B_0^2 L^2 v_0^2}{R}, leading them straight to the trap Option A.

They fail to recognize that the transducer acts as an active AC power source driven by the light energy.

Because the transformer EMF fluctuates symmetrically, it contributes zero net average force against the constant velocity, but its RMS value contributes significantly to the i2Ri^2 R Joule heating.

The problem demands a rigorous, first-principles application of Faraday's Law and Joule's Law rather than a misapplied global energy conservation shortcut.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterWave Optics - Class 12
ConceptMalus's Law
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree