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Question #42950

Difficulty: 8/10 | 🟢 Free

The Question

An infinitely long cylindrical hard magnetic core of radius RR (in meters) has a frozen-in, non-uniform radial magnetization given by M⃗=M0(rR)r^\vec{M} = M_0 \left(\frac{r}{R}\right) \hat{r}, where rr is the radial distance from the cylinder's central axis, r^\hat{r} is the radial unit vector, and M0M_0 is a positive constant (in A/m\text{A/m}). A straight, thin wire carrying a steady free current II (in Amperes) is placed along the central axis of the cylinder. Which of the following represents the magnitude of the magnetic induction B⃗\vec{B} (in Teslas) at a radial distance r=R2r = \frac{R}{2} inside the core? (Assume vacuum permeability is μ0\mu_0 in T⋅m/A\text{T}\cdot\text{m/A})

Options

  • A.

    μ0IπR\frac{\mu_0 I}{\pi R}

  • B.

    (μ0IπR)2+(μ0M02)2\sqrt{\left(\frac{\mu_0 I}{\pi R}\right)^2 + \left(\frac{\mu_0 M_0}{2}\right)^2}

  • C.

    μ0IπR+μ0M02\frac{\mu_0 I}{\pi R} + \frac{\mu_0 M_0}{2}

  • D.

    (μ0IπR)2+(μ0M0)2\sqrt{\left(\frac{\mu_0 I}{\pi R}\right)^2 + (\mu_0 M_0)^2}

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Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Variable_Constraint

Develop pure symbolic logic skills by mastering algebraic constraints without relying on numerical data.

Concepts Behind This Question

Superposition of Magnetic Fields|Soft vs Hard Magnetic Materials|Integration

Why This Question Is Tricky

Common Mistakes

This question tests the fundamental distinction between the magnetic induction (B⃗\vec{B}) and the magnetic field intensity (H⃗\vec{H}) in the presence of hard magnetic materials.

A common trap is for students to misapply the superposition principle by assuming the total B⃗\vec{B}-field is simply the vector sum of the field due to the free current and μ0M⃗\mu_0 \vec{M}.

This incorrectly yields a non-zero radial B⃗\vec{B}-field component (leading to Option B).

By enforcing Gauss's Law for Magnetism (∇⋅B⃗=0\nabla \cdot \vec{B} = 0), students must recognize that a purely radial, frozen-in magnetization generates a corresponding demagnetizing H⃗\vec{H}-field (Hr=−MrH_r = -M_r) such that the radial B⃗\vec{B}-field remains strictly zero.

The problem eliminates candidates who rely on rote formulas without checking Maxwell's divergence conditions.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterMagnetism and Matter - Class 12
ConceptSuperposition of Magnetic Fields
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree