Difference between revisions of "Spinning Charged Ring Model of Elementary Particles"
Jump to navigation
Jump to search
(Imported from text file) |
(Imported from text file) |
||
| Line 12: | Line 12: | ||
==Abstract== | ==Abstract== | ||
| − | The spinning charged ring model that yields correct electron characteristics is proposed here for the proton, positron and antiproton. The ring with electrostatic charge <em>e</em> spins with tangential velocity <em>c,</em> giving the charged elementary particles constant and identical values of magnetic flux. For all four particles, the approrpiate radii <em>R</em> and half-thickness <em>r</em> of the ring can be chosen to yield the observed spins, magnetic moments, sizes and masses.[[Category:Scientific Paper]] | + | The spinning charged ring model that yields correct electron characteristics is proposed here for the proton, positron and antiproton. The ring with electrostatic charge <em>e</em> spins with tangential velocity <em>c,</em> giving the charged elementary particles constant and identical values of magnetic flux. For all four particles, the approrpiate radii <em>R</em> and half-thickness <em>r</em> of the ring can be chosen to yield the observed spins, magnetic moments, sizes and masses. |
| + | |||
| + | [[Category:Scientific Paper|spinning charged ring model elementary particles]] | ||
[[Category:New Energy]] | [[Category:New Energy]] | ||
Revision as of 11:06, 1 January 2017
| Scientific Paper | |
|---|---|
| Title | Spinning Charged Ring Model of Elementary Particles |
| Author(s) | David L Bergman |
| Keywords | spinning charged ring model, elementary particles, magnetic moments |
| Published | 1991 |
| Journal | Galilean Electrodynamics |
| Volume | 2 |
| Number | 2 |
| Pages | 30-32 |
Abstract
The spinning charged ring model that yields correct electron characteristics is proposed here for the proton, positron and antiproton. The ring with electrostatic charge e spins with tangential velocity c, giving the charged elementary particles constant and identical values of magnetic flux. For all four particles, the approrpiate radii R and half-thickness r of the ring can be chosen to yield the observed spins, magnetic moments, sizes and masses.
