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Question #43292

Difficulty: 8/10 | 🟢 Free

The Question

A magnetic needle of moment of inertia II and magnetic dipole moment MM is suspended horizontally by a uniform wire of length LL and radius rr in a uniform horizontal magnetic field BB. The needle undergoes small angular oscillations in the horizontal plane. Initially, the torsional restoring torque per unit radian of the wire is exactly equal to the magnetic restoring torque per unit radian. The temperature of the entire system is then increased by a small amount Δθ\Delta \theta. The coefficient of linear expansion of the needle is α1\alpha_1, and that of the suspension wire is α2\alpha_2. The shear modulus of the wire decreases with temperature as η=η0(1−γΔθ)\eta = \eta_0(1 - \gamma \Delta \theta), and the magnetic moment of the needle decreases as M=M0(1−δΔθ)M = M_0(1 - \delta \Delta \theta). Assuming Δθ\Delta \theta is small enough that higher-order terms are negligible, what is the fractional change in the time period of oscillation, ΔTpTp\frac{\Delta T_p}{T_p}?

Options

  • A.

    (α1−34α2+14γ+14δ)Δθ\left( \alpha_1 - \frac{3}{4}\alpha_2 + \frac{1}{4}\gamma + \frac{1}{4}\delta \right) \Delta \theta

  • B.

    (α1−32α2+12γ)Δθ\left( \alpha_1 - \frac{3}{2}\alpha_2 + \frac{1}{2}\gamma \right) \Delta \theta

  • C.

    (α1+14γ+14δ)Δθ\left( \alpha_1 + \frac{1}{4}\gamma + \frac{1}{4}\delta \right) \Delta \theta

  • D.

    (2α1−32α2+12γ+12δ)Δθ\left( 2\alpha_1 - \frac{3}{2}\alpha_2 + \frac{1}{2}\gamma + \frac{1}{2}\delta \right) \Delta \theta

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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

Tangent Galvanometer Principle|Torsional Oscillations|Thermal Expansion of Area and Volume

Why This Question Is Tricky

Common Mistakes

This question tests the synthesis of rotational dynamics, magnetism, and thermal expansion.

The primary trap lies in the formulation of the effective restoring torque.

Students frequently make two critical errors: (1) They assume the restoring torque is purely magnetic or purely torsional, ignoring that Ceff=Ct+CmC_{eff} = C_t + C_m, which introduces a crucial factor of 1/21/2 in the fractional change of the combined constant. (2) They neglect the geometric thermal expansion of the suspension wire (r4/Lr^4/L dependence), erroneously assuming the torsional constant only changes due to the temperature dependence of the shear modulus (η\eta).

This forces a rigorous application of binomial approximations across multiple coupled physical domains.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterMagnetism and Matter - Class 12
ConceptTangent Galvanometer Principle
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree