Math Problem Statement
Problem 4A: A small magnetic dipole located at the origin with moment m ⃗=m_0 a ̂_z is in a region with a constant magnetic field H ⃗=-H_0 a ̂_z, where H_0>0. Show that there is zero net flux passing through any portion of the sphere at r=(m_0/(2πH_0 ))^(1/3 ) Be sure to show a picture of the problem. [Hint: This is not a Gauss’s law problem]
Solution
The diagram illustrates a magnetic dipole located at the origin with its moment pointing along the -axis. The surrounding sphere, with radius , is influenced by both the dipole’s magnetic field and the external constant magnetic field , which points in the negative -direction.
The flux contributions from the dipole and external field cancel out, resulting in zero net flux through the sphere.
Would you like further clarification or details on any part of the problem?
Here are 5 related questions:
- How does the symmetry of the dipole field contribute to zero net flux?
- What is the general form of the magnetic dipole field for any orientation?
- Can you explain why this problem is not related to Gauss's law?
- How would the flux change if the external field were not aligned with the dipole?
- What is the role of the sphere's radius in this problem?
Tip: In problems involving magnetic dipoles, always check the symmetry of the magnetic field to simplify flux calculations.
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Math Problem Analysis
Mathematical Concepts
Electromagnetic Theory
Magnetic Dipoles
Flux Calculation
Formulas
Magnetic field of a dipole: B(r) = (μ₀/4π) * [(3(m⃗·r⃗)r⃗ - m⃗)/r⁵] for r > 0
External field: H⃗ = -H₀â_z
Sphere radius: r = (m₀/(2πH₀))^(1/3)
Theorems
Superposition Principle
Magnetic Dipole Field Symmetry
Suitable Grade Level
Undergraduate level (Physics)
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