Maxwell's Electrodynamics without Special Relativity Theory (Part III): Difference between revisions
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It is shown that Maxwell's electrodynamics without the velocity restriction has the spinor form for the group V(4), which is (U(1) x SU(2)) x (U(1) x SU(2)). In this model, Newton's space-time is used with Minkowski's space-time and with Euclid's super-light space-time, which follow from the dynamic equations and the connections between the fields and inductions. | It is shown that Maxwell's electrodynamics without the velocity restriction has the spinor form for the group V(4), which is (U(1) x SU(2)) x (U(1) x SU(2)). In this model, Newton's space-time is used with Minkowski's space-time and with Euclid's super-light space-time, which follow from the dynamic equations and the connections between the fields and inductions. | ||
[[Category:Scientific Paper]] | [[Category:Scientific Paper|maxwell 's electrodynamics special relativity theory iii]] | ||
[[Category:Relativity]] | [[Category:Relativity]] | ||
Revision as of 13:40, 1 January 2017
| Scientific Paper | |
|---|---|
| Title | Maxwell\'s Electrodynamics without Special Relativity Theory (Part III) |
| Author(s) | Victor N Barykin |
| Published | 2004 |
| Journal | Galilean Electrodynamics |
| Volume | 15 |
| Number | 3 |
| Pages | 48-50 |
Abstract
It is shown that Maxwell's electrodynamics without the velocity restriction has the spinor form for the group V(4), which is (U(1) x SU(2)) x (U(1) x SU(2)). In this model, Newton's space-time is used with Minkowski's space-time and with Euclid's super-light space-time, which follow from the dynamic equations and the connections between the fields and inductions.