Difference between revisions of "Testing the Boundary Conditions of General Relativity Near the Earth-Sun Saddle Point"

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==Abstract==
 
==Abstract==
  
We suggest that a satellite with a stable atomic clock on board be sent through the Earth-Sun gravitational saddle point to experimentally determine whether Nature prefers static solutions of the field equations of General Relativity, such as the standard Schwarzschild solution, or whether Nature prefers equivalent non-static solutions. This is a test of the boundary conditions of General Relativity rather than of the field equations. The fractional difference in clock rates between the two possibilities is a part in a hundred million. This is a large and easily measurable effect.[[Category:Scientific Paper]]
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We suggest that a satellite with a stable atomic clock on board be sent through the Earth-Sun gravitational saddle point to experimentally determine whether Nature prefers static solutions of the field equations of General Relativity, such as the standard Schwarzschild solution, or whether Nature prefers equivalent non-static solutions. This is a test of the boundary conditions of General Relativity rather than of the field equations. The fractional difference in clock rates between the two possibilities is a part in a hundred million. This is a large and easily measurable effect.
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[[Category:Scientific Paper|testing boundary conditions general relativity near earth-sun saddle point]]
  
 
[[Category:Relativity]]
 
[[Category:Relativity]]

Revision as of 11:09, 1 January 2017

Scientific Paper
Title Testing the Boundary Conditions of General Relativity Near the Earth-Sun Saddle Point
Author(s) Thomas D Martin
Keywords {{{keywords}}}
Journal None
No. of pages 10

Abstract

We suggest that a satellite with a stable atomic clock on board be sent through the Earth-Sun gravitational saddle point to experimentally determine whether Nature prefers static solutions of the field equations of General Relativity, such as the standard Schwarzschild solution, or whether Nature prefers equivalent non-static solutions. This is a test of the boundary conditions of General Relativity rather than of the field equations. The fractional difference in clock rates between the two possibilities is a part in a hundred million. This is a large and easily measurable effect.