Calculating Magnetic Dipole Moment of a Sphere

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Homework Help Overview

The problem involves calculating the magnetic dipole moment of a uniformly charged solid sphere that is spinning. The context includes the relationship between charge density and the magnetic dipole moment, as well as the transition from a disk to a sphere in terms of their respective moments.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the appropriate charge density to use in the context of the magnetic dipole moment, questioning the transition from the moment of a disk to that of a solid sphere. There are attempts to clarify the relationship between different geometries and their respective charge distributions.

Discussion Status

The discussion is active, with participants providing hints and exploring the correct expressions for charge density. There is an ongoing examination of the integral setup and the relationships between variables, though no consensus has been reached on the final formulation.

Contextual Notes

Participants are navigating the complexities of integrating over a solid sphere and the implications of using different charge density definitions. The original poster's approach is being scrutinized for accuracy in the context of the problem's requirements.

ehrenfest
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[SOLVED] Griffiths 5.58

Homework Statement


A uniformly charged solid sphere of radius R carries a total charge Q, and is set spinning with angular velocity \omega.

What is the magnetic dipole moment of the sphere.

Homework Equations


The Attempt at a Solution


The magnetic dipole moment of a disk is

[tex](1/4) r^4 \sigma \pi \omega[/tex]

Why does

[tex]\int_0^{\pi} (Rd\theta) ((1/4) R^4 \sin^4 \theta \sigma \pi \omega)[/tex]

with [itex]\sigma[/itex] replaced by [itex]3Q/(4 \pi R^3)[/itex] not give the correct answer?
 
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I'd imagine that the sigma in the dipole moment of a disk is a charge density per area.
 
genneth said:
I'd imagine that the sigma in the dipole moment of a disk is a charge density per area.

So what is \sigma replaced with here? How do I get the moment for a solid sphere from the moment for a disk?

The analogous idea worked to get the moment of a disk from the moment of a ring which is kind of confusing!
 
Last edited:
There's nothing wrong with the idea. Here's a hint: each disc contains dz * \rho charge, where \rho is the charge per unit volume.
 
isn't dz = Rd\theta ?
 
No. Try [tex]r \sin \theta\,d\theta[/tex]
 
[tex]z = R\cos \theta[/tex] so [tex]dz = - R \sin \theta d\theta[/tex] so the correct integral is

[tex] = - \int_0^{\pi} ( \rho R \sin \theta d\theta) ((1/4) R^4 \sin^4 \theta \pi \omega)[/tex]

right?
 
Last edited:

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