In reply to  Frederick Sparber's message of Sat, 4 Mar 2006
20:00:16 -0700:
Hi,
[snip]
>Robin.
>
>The closest shape for spin and the moment of inertia ( I ) to meet
> mvr = h/2(pi) = I * 2(pi)f is a flat-wavy disk particle I = 1/2 MR^2
>or standing on edge MR^2 
>
>An abbreviated list of moments of inertia:
>
>http://en.wikipedia.org/wiki/List_of_moments_of_inertia
>
>Or You can figure out ( I ) for a torus from this. :-)
>
>http://scienceworld.wolfram.com/physics/MomentofInertiaTorus.html

This is for a solid torus, and I'm not sure whether the mass is
inside, on, or outside the torus. Nevertheless, taking it at face
value, one would only get a difference in angular momentum of 2
parts in a billion, assuming a torus with the dimensions given,
and I think that's probably near the limit of current measurements
anyway.

However I also wonder how anyone knows that the angular momentum
actually is h/2xPi? I.e. how is it measured, and which geometrical
assumptions are applied to the measurement? (i.e. that value
appears to come from assuming the electron is a point particle
spinning around at the Bohr radius).
[snip]
Regards,

Robin van Spaandonk

http://users.bigpond.net.au/rvanspaa/

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Cooperation provides the means.

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