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Question #43263

Difficulty: 8/10 | 🟢 Free

The Question

A rigid, non-conducting thin rod of mass MM and length LL is hinged frictionlessly at the origin (0,0)(0,0) and is free to rotate in the xyxy-plane. The rod has a non-uniform linear mass density λ(x)=2ML2x\lambda(x) = \frac{2M}{L^2}x, where xx is the distance from the hinge. It possesses a permanent magnetic dipole moment of magnitude μ\mu, directed along its length from the hinge to the free end. The rod initially hangs at rest vertically downwards along the −j^-\hat{j} axis. A uniform, constant magnetic field B⃗0=B0j^\vec{B}_0 = B_0 \hat{j} exists in the region, and gravity acts along −j^-\hat{j}. A short magnetic field pulse B⃗pulse(t)=Bp(t)i^\vec{B}_{pulse}(t) = B_p(t) \hat{i} is applied for a negligible duration Δt\Delta t, such that ∫0ΔtBp(t)dt=β\int_0^{\Delta t} B_p(t) dt = \beta. If the rod swings upwards and comes to instantaneous rest exactly at the horizontal position (+i^+\hat{i} axis), which of the following gives the value of β2\beta^2? (Assume 23MgL>μB0\frac{2}{3} M g L > \mu B_0)

Options

  • A.

    ML2μ2(23MgL−μB0)\frac{M L^2}{\mu^2} \left( \frac{2}{3} M g L - \mu B_0 \right)

  • B.

    ML2μ2(23MgL+μB0)\frac{M L^2}{\mu^2} \left( \frac{2}{3} M g L + \mu B_0 \right)

  • C.

    ML2μ2(13MgL−23μB0)\frac{M L^2}{\mu^2} \left( \frac{1}{3} M g L - \frac{2}{3} \mu B_0 \right)

  • D.

    2M3gL33μ2\frac{2 M^3 g L^3}{3 \mu^2}

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Correct Answer

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

Torque and Potential Energy in B-Field|Physical Pendulum Inertia|Work-Energy Theorem for Rotation

Why This Question Is Tricky

Common Mistakes

This question tests the integration of impulsive torques with the rotational work-energy theorem in a multi-field environment.

A primary trap is blindly using standard uniform rod formulas (I=13ML2I = \frac{1}{3}ML^2 and xcm=L/2x_{cm} = L/2), which ignores the explicit non-uniform mass distribution λ(x)\lambda(x) and leads to incorrect kinetic and potential energy terms.

Additionally, students often miscalculate the magnetic potential energy or its sign; because the dipole is initially anti-parallel to the background field, the constant magnetic field does positive work as the rod swings up.

Failing to account for this positive magnetic work, or ignoring the constant field entirely during the swing phase, leads directly to the distractor options.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterMagnetism and Matter - Class 12
ConceptTorque and Potential Energy in B-Field
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree