The Substratum Origin of Relativistic Effects: Difference between revisions
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| published = 1993 | | published = 1993 | ||
| journal = [[Galilean Electrodynamics]] | | journal = [[Galilean Electrodynamics]] | ||
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| pages = 11-14 | | pages = 11-14 | ||
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==Abstract== | ==Abstract== | ||
The Lorentz contraction and other "relativistic" effects can be regarded as the phenomenology of a solid substratum. Particles of matter are modeled by the point defects (singularities) of this medium. Thus within the linear-elastic range no sign of the substratum, such as aether entrainment, can be detected experimentally. | The Lorentz contraction and other "relativistic" effects can be regarded as the phenomenology of a solid substratum. Particles of matter are modeled by the point defects (singularities) of this medium. Thus within the linear-elastic range no sign of the substratum, such as aether entrainment, can be detected experimentally. | ||
[[Category:Relativity]] | [[Category:Scientific Paper|substratum origin relativistic effects]] | ||
[[Category:Relativity|substratum origin relativistic effects]] | |||
Latest revision as of 09:31, 21 July 2026
| Scientific Paper | |
|---|---|
| Title | The Substratum Origin of Relativistic Effects |
| Author(s) | Valery P Dmitriyev |
| Keywords | Lorentz contraction, relativistic effects, solid substratum, matter, aether entrainment |
| Published | 1993 |
| Journal | Galilean Electrodynamics |
| Volume | 4 |
| Number | 1 |
| Pages | 11-14 |
Abstract
The Lorentz contraction and other "relativistic" effects can be regarded as the phenomenology of a solid substratum. Particles of matter are modeled by the point defects (singularities) of this medium. Thus within the linear-elastic range no sign of the substratum, such as aether entrainment, can be detected experimentally.