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Question #43683

Difficulty: 8/10 | 🟢 Free

The Question

A uniform conducting rod of mass MM (kg) and length LL (m) is pivoted at one end and rotates in a horizontal plane. Its free end slides on a frictionless, perfectly conducting circular ring of radius LL. A uniform vertical magnetic field BB (T) is applied perpendicular to the plane of rotation. A stationary resistor of resistance RR (Ω\Omega) connects the pivot and the ring. The rod is composed of a radioactive material with a decay constant λ\lambda (s−1^{-1}). The energy released from the radioactive decay is continuously and entirely converted into mechanical power that drives the rotation of the rod. The initial total available decay energy if all nuclei were to decay is E0E_0 (J). Assuming the mass MM of the rod remains practically constant, and the rod starts from rest at t=0t=0, at what time tmt_m (s) will the angular velocity of the rod reach its maximum value?

Options

  • A.

    2RM3B2L2−2RMλln⁡(3B2L22RMλ)\frac{2RM}{3B^2L^2 - 2RM\lambda} \ln\left( \frac{3B^2L^2}{2RM\lambda} \right)

  • B.

    2RMB2L2−2RMλln⁡(B2L22RMλ)\frac{2RM}{B^2L^2 - 2RM\lambda} \ln\left( \frac{B^2L^2}{2RM\lambda} \right)

  • C.

    RM6B2L2−RMλln⁡(6B2L2RMλ)\frac{RM}{6B^2L^2 - RM\lambda} \ln\left( \frac{6B^2L^2}{RM\lambda} \right)

  • D.

    3RM2B2L2−3RMλln⁡(2B2L23RMλ)\frac{3RM}{2B^2L^2 - 3RM\lambda} \ln\left( \frac{2B^2L^2}{3RM\lambda} \right)

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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

Mass Defect vs. Binding Energy|Motional EMF in Rotating Rods|Lenz’s Law Energy Conservation

Why This Question Is Tricky

Common Mistakes

This question tests the student's ability to synthesize modern physics (radioactive decay power) with electromagnetic induction and rigid body dynamics.

The primary trap lies in the misapplication of the Work-Energy Theorem: students often incorrectly assume a steady-state condition (Pgen=PdissP_{gen} = P_{diss}) from the start, ignoring the inertial term (dKdt\frac{dK}{dt}) which dictates the transient response.

Secondary traps involve incorrect formulations of the motional EMF for a rotating rod (forgetting the 1/21/2 factor, leading to Option C) or using the wrong moment of inertia for a rod pivoted at one end (using ML2ML^2 instead of ML2/3ML^2/3, leading to Option B).

The problem requires setting up and solving a first-order linear differential equation to find the exact time of maximum kinetic energy.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterNuclei - Class 12
ConceptMass Defect vs. Binding Energy
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree