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Question #43034

Difficulty: 8/10 | 🟢 Free

The Question

A moving coil galvanometer consists of a coil of NN turns and area AA, suspended such that it can rotate freely about the zz-axis. It is placed in a permanent radial magnetic field of constant magnitude B0B_0. The torsional constant of the suspension is CC. When no current flows, the coil is in equilibrium and its area vector points along the positive xx-axis. When a steady current I0I_0 is passed through the coil, its area vector deflects by an angle θ0=60∘\theta_0 = 60^\circ towards the positive yy-axis to reach a new equilibrium.

An infinite flat sheet carrying a uniform surface current density K⃗=4B0μ0k^\vec{K} = \frac{4 B_0}{\mu_0} \hat{k} is now placed in the yzyz-plane at x=−dx = -d (where d>0d > 0). The galvanometer is located at the origin. Assume the galvanometer components do not distort the magnetic field produced by the sheet.

A new steady current I′I' is passed through the galvanometer, and it is observed that the coil deflects by the exact same angle θ0=60∘\theta_0 = 60^\circ towards the positive yy-axis. Find the ratio I′I0\frac{I'}{I_0}.

Options

  • A.

    12\frac{1}{2}

  • B.

    13\frac{1}{3}

  • C.

    11+3\frac{1}{1 + \sqrt{3}}

  • D.

    15\frac{1}{\sqrt{5}}

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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

Galvanometer Sensitivity Logic|Field due to Infinite Sheet|Superposition Principle

Why This Question Is Tricky

Common Mistakes

This question tests the principle of superposition of magnetic fields and the vector nature of magnetic torque in a moving coil galvanometer.

Students often memorize the standard formula I=CθNABI = \frac{C\theta}{NAB} assuming the magnetic field is purely radial and always perpendicular to the area vector.

The trap lies in failing to recognize that an external uniform magnetic field introduces an angle-dependent torque (M⃗×B⃗ext\vec{M} \times \vec{B}_{ext}).

By superimposing a uniform field from an infinite sheet, the total restoring torque becomes a function of the deflection angle's cosine, breaking the linear sensitivity of the galvanometer and requiring a fundamental free-body diagram of torques to solve.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterMoving Charges and Magnetism - Class 12
ConceptGalvanometer Sensitivity Logic
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree