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{{Infobox paper
{{Infobox paper
| title = Maxwell\'s Electrodynamics without Special Relativity Theory (Part VI)
| 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 = [[19]]
| volume = 19
| number = [[S1]]
| number = S1
| pages = 18-21
| pages = 18-21
}}
}}
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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.
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.


[[Category:Scientific Paper]]
[[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
TitleMaxwell's Electrodynamics without Special Relativity Theory (Part VI)
Author(s)Victor N Barykin
Keywordsspecial relativity theory, electrodynamics, Maxwell, electromagnetic field
Published2008
JournalGalilean Electrodynamics
Volume19
NumberS1
Pages18-21

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.