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Question #42754

Difficulty: 8/10 | 🟢 Free

The Question

A composite point dipole consisting of an electric dipole moment p⃗\vec{p} and a magnetic dipole moment m⃗\vec{m} is located at position r⃗=di^\vec{r} = d \hat{i}. A point charge +Q+Q is fixed at the origin. A non-uniform external magnetic field B⃗=α(xi^−yj^)\vec{B} = \alpha (x \hat{i} - y \hat{j}) exists in the region, where α\alpha is a positive constant. The dipole moments are parallel to each other (p⃗∥m⃗\vec{p} \parallel \vec{m}) and lie in the xyxy-plane, making an angle θ\theta with the positive xx-axis. An external agent rotates the composite dipole quasi-statically about its center of mass (which remains fixed at r⃗=di^\vec{r} = d \hat{i}) from θ=0\theta = 0 to θ=π/2\theta = \pi/2. Let WW be the total work done by the external agent during this rotation, and let ∣τ⃗O∣|\vec{\tau}_O| be the magnitude of the net torque exerted by the electric and magnetic fields on the composite dipole about the origin at an arbitrary angle θ\theta. Which of the following gives the correct expressions for WW and ∣τ⃗O∣|\vec{\tau}_O|?

Options

  • A.

    W=pQ4πϵ0d2+mαd;∣τ⃗O∣=2mαdsin⁡θW = \frac{pQ}{4\pi\epsilon_0 d^2} + m \alpha d \quad ; \quad |\vec{\tau}_O| = 2 m \alpha d \sin\theta

  • B.

    W=pQ4πϵ0d2+mαd;∣τ⃗O∣=(pQ4πϵ0d2+mαd)sin⁡θW = \frac{pQ}{4\pi\epsilon_0 d^2} + m \alpha d \quad ; \quad |\vec{\tau}_O| = \left( \frac{pQ}{4\pi\epsilon_0 d^2} + m \alpha d \right) \sin\theta

  • C.

    W=pQ2πϵ0d2+2mαd;∣τ⃗O∣=2mαdsin⁡θW = \frac{pQ}{2\pi\epsilon_0 d^2} + 2 m \alpha d \quad ; \quad |\vec{\tau}_O| = 2 m \alpha d \sin\theta

  • D.

    W=pQ4πϵ0d2+mαd;∣τ⃗O∣=mαdsin⁡θW = \frac{pQ}{4\pi\epsilon_0 d^2} + m \alpha d \quad ; \quad |\vec{\tau}_O| = m \alpha d \sin\theta

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Step-by-Step Solution

Explanation

How the Examiner Thinks

Multi-Concept_Bridge

Master problems that require linking physics and math concepts to solve complex competitive questions.

Concepts Behind This Question

Work Done in Rotating Dipole|Magnetic Dipole Moment Orientation|Integration

Why This Question Is Tricky

Common Mistakes

This question tests the calculation of work and torque for dipoles in non-uniform fields.

The primary trap lies in evaluating the net torque about the origin.

Students frequently misapply the torque formula by assuming τ⃗O=p⃗×E⃗+m⃗×B⃗\vec{\tau}_O = \vec{p} \times \vec{E} + \vec{m} \times \vec{B}, forgetting that the spatial gradient of the fields exerts a net translational force F⃗=(p⃗⋅∇)E⃗+(m⃗⋅∇)B⃗\vec{F} = (\vec{p} \cdot \nabla)\vec{E} + (\vec{m} \cdot \nabla)\vec{B} on the dipoles.

This force creates an additional torque r⃗×F⃗\vec{r} \times \vec{F} about the origin.

A secondary trap is failing to recognize that the electric torque about the origin perfectly cancels out due to the central nature of the point charge's field, while the magnetic torque components add up, leading to the non-intuitive factor of 2 in the final magnetic torque expression.

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Question Information

SubjectPhysics
ChapterElectrostatic Potential and Capacitance - Class 12
ConceptWork Done in Rotating Dipole
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree