Gyromagnetic Ratio: Q/2M Explained

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Discussion Overview

The discussion revolves around the gyromagnetic ratio, specifically the relationship between the gyromagnetic ratio of a rotating circular loop and that of a uniform rotating sphere. Participants explore theoretical implications, mathematical reasoning, and conceptual clarifications related to the gyromagnetic ratio defined as g = Q/2M.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants express confusion regarding how the gyromagnetic ratio for a rotating circular loop implies the same ratio for a uniform rotating sphere.
  • Questions are raised about whether the gyromagnetic ratio of the rotating loop depends on the size of the loop, with some asserting that it does not.
  • One participant suggests that the dipole moment of a rotating spherically symmetric charge distribution can be conceptualized as the sum of contributions from infinitesimal loops, leading to concerns about the total dipole moment being infinite.
  • Another participant challenges the idea of an infinite dipole moment, referencing established texts and suggesting that the calculation should yield a finite result.
  • There is a discussion about the reasoning presented in Griffiths' text, which implies that the gyromagnetic ratio for a uniform spinning sphere can be derived from the result for a ring.
  • Some participants share insights about integrating to find the gyromagnetic ratio for solids of revolution, noting that the integrals for magnetic moment and angular momentum cancel in the ratio.
  • Concerns are raised about the generalizability of the results to other shapes, with one participant expressing skepticism about whether the outcome is coincidental.

Areas of Agreement / Disagreement

Participants do not reach a consensus; there are competing views regarding the implications of the gyromagnetic ratio for different geometries and the validity of the reasoning presented. Some participants challenge each other's interpretations and calculations without resolving the disagreements.

Contextual Notes

Participants express uncertainty regarding the assumptions made in their calculations, particularly concerning the treatment of charge and mass distributions in the context of the gyromagnetic ratio.

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:

[tex]\frac{dQ}{dM} = \frac{dQ/dV}{dM/dV} = \frac{\rho_q}{\rho_m} = \frac{Q}{M}[/tex]
 
  • #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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