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Question #43096

Difficulty: 8/10 | 🟢 Free

The Question

A small circular loop of radius aa is placed at the origin in the xyxy-plane and carries an alternating current I(t)=I0cos⁡(ωt)I(t) = I_0 \cos(\omega t). This loop acts as an oscillating magnetic dipole. Consider a point PP in the xyxy-plane at a distance rr from the origin (r≫ar \gg a). The displacement current density J⃗d\vec{J}_d at point PP due to the electromagnetic fields of the dipole can be expressed in the form J⃗d=Jmaxcos⁡(ωt+ϕ)ϕ^\vec{J}_d = J_{\text{max}} \cos(\omega t + \phi) \hat{\phi}, where ϕ^\hat{\phi} is the azimuthal unit vector, Jmax>0J_{\text{max}} > 0 is a time-independent scalar amplitude, and ϕ\phi is the phase difference relative to the source current I(t)I(t). Given that the speed of light in vacuum is cc, which of the following expressions correctly represents the phase difference ϕ\phi?

Options

  • A.

    tan⁡−1(ωrc)−ωrc\tan^{-1}\left(\frac{\omega r}{c}\right) - \frac{\omega r}{c}

  • B.

    −ωrc-\frac{\omega r}{c}

  • C.

    tan⁡−1(cωr)−ωrc\tan^{-1}\left(\frac{c}{\omega r}\right) - \frac{\omega r}{c}

  • D.

    ωrc−tan⁡−1(ωrc)\frac{\omega r}{c} - \tan^{-1}\left(\frac{\omega r}{c}\right)

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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

Phase Relationship|Displacement Current Source|Magnetic Dipole Moment of Revolving Electron

Why This Question Is Tricky

Common Mistakes

This question targets the 'Near-Field Approximation' fallacy and tests the student's understanding of retarded potentials in electrodynamics.

Students often incorrectly assume that the magnetic field of an oscillating dipole is simply the instantaneous Biot-Savart field, which would lead to a phase difference of zero (ignoring retardation entirely).

Even if they account for the time delay t−r/ct - r/c, they might erroneously isolate either the radiation (1/r1/r) term or the quasi-static (1/r21/r^2) term.

By asking for the displacement current phase at an arbitrary distance rr, the student is forced to use the complete retarded vector potential.

The phase shift tan⁡−1(ωr/c)\tan^{-1}(\omega r/c) arises directly from the superposition of these near-field and far-field components, proving that phase synchronization is distance-dependent and that Maxwell's equations do not permit action-at-a-distance.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterElectromagnetic Waves - Class 12
ConceptPhase Relationship
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree