# 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"

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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 []. |

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+ | [[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 [].