Difference between revisions of "Convention in the Definition of Geometry of Space-Time"
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==Abstract== | ==Abstract== | ||
− | A hundred years ago, Poincar? pointed out that relativistic mechanics can be described within different geometries of space-time. This paper assumes the signal method of clock synchronization in pseudo-Euclidean, Euclidean and Galilean geometries, and obtains transformations of coordinates and time for these geometries under general nonstandard clock synchronization. | + | A hundred years ago, Poincar? pointed out that relativistic mechanics can be described within different geometries of space-time. This paper assumes the signal method of clock synchronization in pseudo-Euclidean, Euclidean and Galilean geometries, and obtains transformations of coordinates and time for these geometries under general nonstandard clock synchronization. |
− | [[Category:Relativity]] | + | [[Category:Scientific Paper|convention definition geometry space-time]] |
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+ | [[Category:Relativity|convention definition geometry space-time]] |
Latest revision as of 19:24, 1 January 2017
Scientific Paper | |
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Title | Convention in the Definition of Geometry of Space-Time |
Author(s) | R G Zaripov |
Keywords | simultaneity, geometry relativity, transformation |
Published | 2000 |
Journal | Galilean Electrodynamics |
Volume | 11 |
Number | 4 |
Pages | 63-68 |
Abstract
A hundred years ago, Poincar? pointed out that relativistic mechanics can be described within different geometries of space-time. This paper assumes the signal method of clock synchronization in pseudo-Euclidean, Euclidean and Galilean geometries, and obtains transformations of coordinates and time for these geometries under general nonstandard clock synchronization.