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Question #42830

Difficulty: 8/10 | 🟢 Free

The Question

A rigid insulating rod of length 2a2a has point charges +q+q and −q-q fixed at its ends, forming an electric dipole of moment p⃗\vec{p} (where p=2qap = 2qa). The dipole is placed such that its center is fixed on the axis of a circular loop of radius RR (R≫aR \gg a) carrying a steady counter-clockwise current II. The loop lies in the xyxy-plane with its center at the origin (0,0,0)(0,0,0). The center of the dipole is located at coordinates (0,0,R)(0, 0, R). The dipole is constrained to rotate in the plane z=Rz = R with a constant angular velocity ω⃗=ωk^\vec{\omega} = \omega \hat{k}. A uniform electric field E⃗=E0i^\vec{E} = E_0 \hat{i} is also present in the entire region. At the instant the dipole moment vector is aligned with the positive yy-axis (p⃗=pj^\vec{p} = p \hat{j}), what is the net torque τ⃗\vec{\tau} acting on the dipole about its center? (Assume the magnetic field variation over the length of the dipole is small but non-zero, and account for all spatial components of the magnetic field).

Options

  • A.

    −3μ0Ipa2ω162R2i^−pE0k^-\frac{3 \mu_0 I p a^2 \omega}{16\sqrt{2} R^2} \hat{i} - p E_0 \hat{k}

  • B.

    −pE0k^- p E_0 \hat{k}

  • C.

    +3μ0Ipa2ω162R2i^−pE0k^+\frac{3 \mu_0 I p a^2 \omega}{16\sqrt{2} R^2} \hat{i} - p E_0 \hat{k}

  • D.

    −3μ0Ipa2ω82R2j^−pE0k^-\frac{3 \mu_0 I p a^2 \omega}{8\sqrt{2} R^2} \hat{j} - p E_0 \hat{k}

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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

Dipole in Uniform Field|Magnetic Dipole Moment Orientation|Faraday’s Law Vector Form

Why This Question Is Tricky

Common Mistakes

This question tests the student's ability to transition from pure electrostatics to electrodynamics by placing a rotating electric dipole in a non-uniform magnetic field.

The primary trap is the assumption that a magnetic field exerts no net torque on an electric dipole, leading students to only calculate the electrostatic torque τ⃗=p⃗×E⃗\vec{\tau} = \vec{p} \times \vec{E} (Option B).

Even if students realize the charges are moving and experience a Lorentz force, they often falsely assume the magnetic field on the axis is purely axial (B⃗=Bzk^\vec{B} = B_z \hat{k}).

If Br=0B_r = 0, the magnetic force is purely radial and produces zero torque.

The 'Lethal Collision' occurs because students fail to apply Gauss's Law for Magnetism (∇⋅B⃗=0\nabla \cdot \vec{B} = 0), which dictates that a spatially varying axial field must be accompanied by a radial field component.

This radial component interacts with the azimuthal velocity of the charges to produce a zz-directed force, creating a torque that tilts the dipole out of its plane of rotation.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterElectric Charges and Fields - Class 12
ConceptDipole in Uniform Field
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree