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Question #43445

Difficulty: 8/10 | 🟢 Free

The Question

A cylindrical magnetic material of radius RR and length LL is modeled as having a non-uniform azimuthal volume current density J⃗(r)=J0(rR)2ϕ^\vec{J}(r) = J_0 \left(\frac{r}{R}\right)^2 \hat{\phi}, where rr is the radial distance from the central axis of the cylinder, J0J_0 is a positive constant, and ϕ^\hat{\phi} is the azimuthal unit vector. The cylinder is centered at the origin with its axis along the zz-axis. Which of the following represents the magnitude of the magnetic field BB at a point on the zz-axis at a distance zz from the center, where z≫Lz \gg L and z≫Rz \gg R?

Options

  • A.

    μ0J0LR310z3\frac{\mu_0 J_0 L R^3}{10 z^3}

  • B.

    μ0J0LR36z3\frac{\mu_0 J_0 L R^3}{6 z^3}

  • C.

    μ0J0LR320z3\frac{\mu_0 J_0 L R^3}{20 z^3}

  • D.

    μ0J0LR35z3\frac{\mu_0 J_0 L R^3}{5 z^3}

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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

Bar Magnet as Equivalent Solenoid|Biot-Savart Law Vector Symmetry|Integration

Why This Question Is Tricky

Common Mistakes

This question tests the student's ability to transition from the Biot-Savart law for a simple loop to a volume-distributed current density J(r)J(r), which models non-homogeneous magnetization.

The primary trap lies in incorrectly defining the differential magnetic moment.

Students often calculate the total current Itot=∫J(r)LdrI_{tot} = \int J(r) L dr and mistakenly multiply it by the total cross-sectional area πR2\pi R^2 (yielding the incorrect option B), failing to recognize that the area enclosed by each differential current loop varies with rr.

Another common error is using the equatorial dipole formula instead of the axial one, omitting the factor of 2 (yielding option C).

By requiring the integration of dμ=J(r)⋅πr2⋅dr dzd\mu = J(r) \cdot \pi r^2 \cdot dr\,dz, the problem enforces a rigorous understanding of the superposition principle for magnetic dipoles.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterMagnetism and Matter - Class 12
ConceptBar Magnet as Equivalent Solenoid
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree