Difference between revisions of "The Coulomb Field as the Basic Particle of the Universe"
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| − | Thanks to Coulomb, we have measurable electrostatic and magnetic fields that stand alone. That is, when they are not in motion. Given motion, the two fields form a union - orthogonally to each other - which we call an electromagnetic field (e.m. for short). Nieto & Goldhaber, experimenters (among others), determined the approximate mass of these fields. (See Scientific American, May, 1976, The Mass of the Photon, by Nieto & Goldhaber) . As their experiment progressed over time, they refined their technique such that the result became progressively smaller - and eventually approached very close to the figure given here. There were anomalies of the curve caused by their examining other fields than the coulomb fields. These should be ignored.[[Category:Scientific Paper]] | + | Thanks to Coulomb, we have measurable electrostatic and magnetic fields that stand alone. That is, when they are not in motion. Given motion, the two fields form a union - orthogonally to each other - which we call an electromagnetic field (e.m. for short). Nieto & Goldhaber, experimenters (among others), determined the approximate mass of these fields. (See Scientific American, May, 1976, The Mass of the Photon, by Nieto & Goldhaber) . As their experiment progressed over time, they refined their technique such that the result became progressively smaller - and eventually approached very close to the figure given here. There were anomalies of the curve caused by their examining other fields than the coulomb fields. These should be ignored. |
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| + | [[Category:Scientific Paper|coulomb field basic particle universe]] | ||
Latest revision as of 11:12, 1 January 2017
| Scientific Paper | |
|---|---|
| Title | The Coulomb Field as the Basic Particle of the Universe |
| Author(s) | Vertner Vergon |
| Keywords | Coulomb |
| Published | 2006 |
| Journal | General Science Journal |
Abstract
Thanks to Coulomb, we have measurable electrostatic and magnetic fields that stand alone. That is, when they are not in motion. Given motion, the two fields form a union - orthogonally to each other - which we call an electromagnetic field (e.m. for short). Nieto & Goldhaber, experimenters (among others), determined the approximate mass of these fields. (See Scientific American, May, 1976, The Mass of the Photon, by Nieto & Goldhaber) . As their experiment progressed over time, they refined their technique such that the result became progressively smaller - and eventually approached very close to the figure given here. There were anomalies of the curve caused by their examining other fields than the coulomb fields. These should be ignored.
