Difference between revisions of "Investigations with Lasers, Atomic Clocks and Computer Calculations of Curved Spacetime and of the Differences Between the Gravitation Theories of Yilmaz and of Einstein"
Jump to navigation
Jump to search
(Imported from text file) |
(Imported from text file) |
||
Line 10: | Line 10: | ||
==Abstract== | ==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 [].[[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 10:35, 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 [].