Maxwell's Electrodynamics without Special Relativity Theory (Part VI): Difference between revisions
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{{Infobox paper | {{Infobox paper | ||
| title = Maxwell | | title = Maxwell's Electrodynamics without Special Relativity Theory (Part VI) | ||
| author = [[Victor N Barykin]] | | author = [[Victor N Barykin]] | ||
| keywords = special relativity theory, electrodynamics, Maxwell, electromagnetic field | |||
| published = 2008 | | published = 2008 | ||
| journal = [[Galilean Electrodynamics]] | | journal = [[Galilean Electrodynamics]] | ||
| volume = | | volume = 19 | ||
| number = | | number = S1 | ||
| pages = 18-21 | | pages = 18-21 | ||
}} | }} | ||
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[[Category:Scientific Paper|maxwell 's electrodynamics special relativity theory vi]] | [[Category:Scientific Paper|maxwell 's electrodynamics special relativity theory vi]] | ||
[[Category:Relativity]] | [[Category:Relativity|maxwell 's electrodynamics special relativity theory vi]] | ||
Latest revision as of 09:36, 21 July 2026
| Scientific Paper | |
|---|---|
| Title | Maxwell's Electrodynamics without Special Relativity Theory (Part VI) |
| Author(s) | Victor N Barykin |
| Keywords | special relativity theory, electrodynamics, Maxwell, electromagnetic field |
| Published | 2008 |
| Journal | Galilean Electrodynamics |
| Volume | 19 |
| Number | S1 |
| Pages | 18-21 |
Abstract
The dynamical influence of the classical experimental equipment at the electromagnetic field is described by the class of the Lorentz's transformations dependent on 0-cohomology group w(x). They act in the space of events SE, which is additional to the Newton's space.