Investigations with Lasers, Atomic Clocks and Computer Calculations of Curved Spacetime and of the Differences Between the Gravitation Theories of Yilmaz and of Einstein: Difference between revisions
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The description of gravitation by curved spacetime is a grand concept due to Albert Einstein. The form of his field equations for the determination of the metric coefficients for a given distribution of matter and field stress-energy is an assumption. The source term (right hand side) of these equations for the Einstein-Hilbert curvature tensor is taken to be the stress-energy tensor [] of all matter and fields except that of the gravitational field itself [].[[Category:Scientific Paper]] | The description of gravitation by curved spacetime is a grand concept due to Albert Einstein. The form of his field equations for the determination of the metric coefficients for a given distribution of matter and field stress-energy is an assumption. The source term (right hand side) of these equations for the Einstein-Hilbert curvature tensor is taken to be the stress-energy tensor [] of all matter and fields except that of the gravitational field itself []. | ||
[[Category:Scientific Paper|investigations lasers atomic clocks calculations curved spacetime differences gravitation theories yilmaz einstein]] | |||
[[Category:Gravity]] | [[Category:Gravity]] | ||
Revision as of 13:35, 1 January 2017
| Scientific Paper | |
|---|---|
| Title | Investigations with Lasers, Atomic Clocks and Computer Calculations of Curved Spacetime and of the Differences Between the Gravitation Theories of Yilmaz and of Einstein |
| Author(s) | Carroll O Alley |
| Keywords | investigations, lasers, atomic clocks, computer calculations, curved spacetime, gravitation theories |
| Published | 1994 |
| Journal | None |
| Pages | 125-137 |
Abstract
The description of gravitation by curved spacetime is a grand concept due to Albert Einstein. The form of his field equations for the determination of the metric coefficients for a given distribution of matter and field stress-energy is an assumption. The source term (right hand side) of these equations for the Einstein-Hilbert curvature tensor is taken to be the stress-energy tensor [] of all matter and fields except that of the gravitational field itself [].