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Question #42492

Difficulty: 8/10 | 🟢 Free

The Question

A smooth circular hoop of mass mm and radius RR is constrained to rotate freely without friction about its vertical diameter. A small bead, also of mass mm, can slide without friction along the hoop. The moment of inertia of the hoop about its vertical diameter is 12mR2\frac{1}{2}mR^2. Initially, the bead is at an angle θ=60∘\theta = 60^\circ from the lowest point, and the entire system rotates freely with an angular velocity ω0=2gR\omega_0 = \sqrt{\frac{2g}{R}}. In this state, the bead is in stable equilibrium and at rest relative to the hoop. The bead is then given a sudden velocity along the hoop towards the lowest point. What is the minimum initial kinetic energy of the bead, measured in the rotating frame of the hoop, required for it to reach the lowest point (θ=0\theta = 0)? (Assume gg is the acceleration due to gravity)

Options

  • A.

    118mgR\frac{11}{8} mgR

  • B.

    14mgR\frac{1}{4} mgR

  • C.

    178mgR\frac{17}{8} mgR

  • D.

    34mgR\frac{3}{4} mgR

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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

Equilibrium Stability|Angular Momentum conservation|Rigid Body Constraints|Vector Cross-Product

Why This Question Is Tricky

Common Mistakes

This question tests the student's ability to analyze the stability and energetics of a rigid body system with a shifting mass distribution (a variable moment of inertia constraint).

The primary trap is assuming that the angular velocity ω\omega remains constant during the bead's motion, which would lead to an incorrect application of the centrifugal potential Vrot=−mgRcos⁡θ−12mω2R2sin⁡2θV_{\text{rot}} = -mgR\cos\theta - \frac{1}{2}m\omega^2 R^2 \sin^2\theta (yielding the trap Option B).

Because the system rotates freely, angular momentum LL is conserved, not ω\omega.

Students must construct the correct effective potential energy Veff(θ)=V(θ)+L22I(θ)V_{\text{eff}}(\theta) = V(\theta) + \frac{L^2}{2I(\theta)} and equate the potential well depth to the required kinetic energy to cross the unstable boundary at the lowest point.

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Question Information

SubjectPhysics
ChapterWork, Energy, and Power - Class 11 Part 1
ConceptEquilibrium Stability
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree