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Question #42368

Difficulty: 8/10 | 🟢 Free

The Question

A block of mass MM rests on a smooth horizontal surface. A uniform rod of mass mm and length LL is hinged at its upper end AA to the block. The lower end BB of the rod is connected to a fixed vertical wall to the right by a horizontal massless inextensible string. Initially, the rod is vertical and the string is taut. A constant horizontal force FF is applied to the block towards the right. Find the tension in the string immediately after the force is applied.

Options

  • A.

    mF2(3M+m)\frac{m F}{2(3M + m)}

  • B.

    2mF6M+m\frac{2 m F}{6M + m}

  • C.

    mF2M+m\frac{m F}{2M + m}

  • D.

    mF3(2M+m)\frac{m F}{3(2M + m)}

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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 about non-fixed axes|Constraint Relations via String Length|Physical Pendulum Inertia

Why This Question Is Tricky

Common Mistakes

This question tests the ability to handle torque in non-inertial frames and constraint relations.

The lethal trap is calculating torque about the moving hinge AA without including the pseudo-force torque (−ma-ma acting at the CM).

Students who ignore the pseudo-force write τA=TL=IAα\tau_A = T L = I_A \alpha, leading to T=ma/3T = ma/3 and an incorrect final answer of 2mF6M+m\frac{2mF}{6M+m}.

The rigorous approach requires either applying the pseudo-force correctly (τA=ma(L/2)−TL=IAα\tau_A = ma(L/2) - TL = I_A \alpha) or recognizing that the constrained bottom end BB (aB=0a_B=0) serves as an instantaneous inertial pivot, drastically simplifying the torque equation.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterSystem of Particles and Rotational Motion - Class 11 Part 1
ConceptTorque about non-fixed axes
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree