Gyromagnetic Ratio: Q/2M Explained

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SUMMARY

The gyromagnetic ratio, defined as the ratio of the magnetic dipole moment to angular momentum, is consistently expressed as g = Q/2M for both rotating circular loops and uniform rotating spheres. The discussion highlights that the dipole moment for a uniformly charged rotating sphere can be derived by integrating over infinitesimal loops, leading to the same ratio. Key texts such as Griffiths, Wangsness, and Jackson provide foundational insights into calculating the dipole moment for such systems. The integrals for magnetic moment and angular momentum cancel out, affirming the universality of the gyromagnetic ratio across solid figures of revolution.

PREREQUISITES
  • Understanding of gyromagnetic ratio and its significance in physics.
  • Familiarity with magnetic dipole moment and angular momentum concepts.
  • Knowledge of integration techniques in physics, particularly for charge distributions.
  • Basic grasp of solid figures of revolution and their properties.
NEXT STEPS
  • Study the derivation of the gyromagnetic ratio in Griffiths' "Introduction to Electrodynamics".
  • Explore the calculation of magnetic moments for various charge distributions in Wangsness' "Electromagnetic Fields".
  • Learn about the application of integrals in determining properties of rotating bodies in Jackson's "Classical Electrodynamics".
  • Investigate the implications of the gyromagnetic ratio in advanced physics topics, such as quantum mechanics and particle physics.
USEFUL FOR

Physicists, electrical engineers, and students studying electromagnetism and classical mechanics will benefit from this discussion, particularly those interested in the properties of rotating charged bodies and their magnetic characteristics.

quasar987
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Hi,

The gyromagnetic ratio is the ratio of the magnetic dipole moment to the angular momentum.

I really don't get how the fact that the gyromagnetic ratio of a rotating circular loop of mass M and charge Q is g = Q/2M implies that the gyromagnetic ratio of a uniform rotating spere is also g = Q/2M!
 
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Points to ponder:

(a) Does the gyromagnetic ratio of the rotating loop depend on the size of the loop?

(b) Can you determine the dipole moment of a rotating spherically symmetric charge distribution by summing over loops?
 
Tide said:
Points to ponder:

(a) Does the gyromagnetic ratio of the rotating loop depend on the size of the loop?

No.

Tide said:
(b) Can you determine the dipole moment of a rotating spherically symmetric charge distribution by summing over loops?

This is exactly what's throwing me off! In principle, since the sphere could be considered as an infinity of circular loops of different sizes, its dipole moment is the sum of all those. But since the sphere is uniform, the ratio of its mass to its charge is the same at every point of it. Hence, the dipole moment of each loops is the same at Q/2M, making the total dipole of the sphere infinite!
 
The dipole moment for a charged rotating sphere is a problem in Griffths, Wangsness and Jackson amongst other texts. It is not infinite, look in some these texts to get an idea on how to calculate it. I think that the easiest manner to go about it is to start with the vector potential for a rotating sphere and go on from there.
 
Griffiths says:

David J. said:
What is the gyromagnetic ratio for a uniform spinnin sphere? [This requires no new calculation; simply decompose the sphere into infinitesimal rings, and apply the result of part (a)

The result of part (a) was of course that g = Q/2M for a ring.

So he seems to be saying that just by reasoning, we can determine that it is the same. I exposed my reasoning to you; what is flawed in it?
 
I did it by integration.

Does anyone know what is the argument that allows one to conclude that the gyromagnetic ratio of any solid of revolution is Q/2M ?
 
You should have gotten a clue from the work you did for the sphere. The integrals for the magnetic moment and angular momentum cancel when you form the ratio! :)
 
quasar987 said:
No.



This is exactly what's throwing me off! ... Hence, the dipole moment of each loops is the same at Q/2M, making the total dipole of the sphere infinite!
No, each loop only has some infinitesimal charge dQ and infinitesimal mass dM.
 
Gokul43201 said:
No, each loop only has some infinitesimal charge dQ and infinitesimal mass dM.

Sure but I'm convinced that nevertheless, their ratio is the same:

\frac{dQ}{dM} = \frac{dQ/dV}{dM/dV} = \frac{\rho_q}{\rho_m} = \frac{Q}{M}
 
  • #10
Tide said:
You should have gotten a clue from the work you did for the sphere. The integrals for the magnetic moment and angular momentum cancel when you form the ratio! :)

For the sphere ok. But that seemed almost like magic you know. There are all these constant that come in from integration and they end up being 1/2 at the end. How do I know it wasn't a big coincidence and that for another random revolution figure, it will be different?

Edit: Ok, now I see it from the integral, by generalizing to an arbitrary volume of revolution, that it will always give Q/2M. Thanks for the hint Tide.
 
Last edited:
  • #11
Quasar,

Any time! :)
 

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