Magnetic Moment to Angular Momentum Ratio

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SUMMARY

The discussion focuses on deriving the ratio of the magnetic moment to angular momentum for an electron modeled as a small spherical shell with mass m and charge e. The conclusion reached is that this ratio is consistently e/2m, regardless of whether the electron is moving in a circular orbit or spinning about a diameter. The calculations provided confirm that both scenarios yield the same result, demonstrating the fundamental relationship between magnetic moment and angular momentum in this context.

PREREQUISITES
  • Understanding of classical electromagnetism, specifically magnetic moments.
  • Familiarity with angular momentum concepts in physics.
  • Knowledge of circular motion and rotational dynamics.
  • Basic calculus for integrating over continuous charge distributions.
NEXT STEPS
  • Explore the derivation of magnetic moments for different charge distributions.
  • Study the implications of angular momentum conservation in electromagnetic systems.
  • Learn about the magnetic field generated by rotating charged spheres.
  • Investigate the applications of magnetic moment to angular momentum ratios in quantum mechanics.
USEFUL FOR

This discussion is beneficial for physics students, educators, and researchers interested in electromagnetism, angular momentum, and the behavior of charged particles in motion.

atomicpedals
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Homework Statement



Suppose that an electron is a small spherical shell of mass m with a charge e spread over its surface. Show that the ratio of the magnetic moment to angular momentum of such an electron should be e/2m whether the electron is a) moving in a circular orbit or b) spinning about a diameter.

2. The attempt at a solution

I'm confident in my reasoning for part a, which is as follows

I=-e/2 pi r = -e me vr/ 2 pi me r2

sin(a) M = IA

M = -e L/ 2 m

which then implies M /L = e/2m.

What has me stuck is how the solution for part b would proceed any differently (other than I'm pretty sure it does proceed differently). Any suggestions as to what I'm not seeing?
 
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for part b how would I find the B field of a uniformly charged rotating sphere?
 
Here is how I went about it in the end:

We can treat a sphere as a collection of infinitesimal rings, so M/L should be the same for a ring as for a sphere. So:

M = IA = (qv/ 2\pir)(\pi r2 )

=(q/2m)(mvr) => M /L = e/2m
 

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