Abstract

We present a Relativistic Newtonian Dynamics ( R N D ) for motion of objects in a gravitational field generated by a moving source. As in General Relativity ( G R ), we assume that objects move by a geodesic with respect to some metric, which is defined by the field. This metric is defined on flat lab spacetime and is derived using only symmetry, the fact that the field propagates with the speed of light, and the Newtonian limit. For a field of a single source, the influenced direction of the field at spacetime point x is defined as the direction from x to the to the position of the source at the retarded time. The metric depends only on this direction and the strength of the field at x. We show that for a static source, the R N D metric is of the same form as the Whitehead metric, and the Schwarzschild metric in Eddington–Finkelstein coordinates. Motion predicted under this model passes all classical tests of G R . Moreover, in this model, the total time for a round trip of light is as predicted by G R , but velocities of light and object and time dilation differ from the G R predictions. For example, light rays propagating toward the massive object do not slow down. The new time dilation prediction could be observed by measuring the relativistic redshift for stars near a black hole and for sungrazing comets. Terrestrial experiments to test speed of light predictions and the relativistic redshift are proposed. The R N D model is similar to Whitehead’s gravitation model for a static field, but its proposed extension to the non-static case is different. This extension uses a complex four-potential description of fields propagating with the speed of light.

Highlights

  • Einstein’s General Relativity (GR) has succeeded in explaining non-classical behavior in astrophysics

  • The metric describes the gravitational field, and, assuming that the field propagates with the speed of light, it is defined by the position of the sources at the retarded time

  • We justify the use of a flat lab spacetime frame, as real astronomical measurements are done with respect to objects far removed from the sources of the field

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Summary

Introduction

Einstein’s General Relativity (GR) has succeeded in explaining non-classical behavior in astrophysics. Whitehead published [4] a relativistic theory of gravity, much simpler than GR and containing no arbitrary parameters This theory is set in Minkowski spacetime, and it is assumed that the motion of any object is by a geodesic with respect to a metric defined on this spacetime. The metric describes the gravitational field, and, assuming that the field propagates with the speed of light, it is defined by the position of the sources at the retarded time. In contrast to Whitehead’s theory, RND makes predictions different from GR for the relativistic redshift. Static gravitational field, RND predicts a different one-way speed of light from that predicted by GR. We propose how to extend RND to a non-static force field This extension is based on the pre-potential and four-potential description on a field propagating with the speed of light, see [24]

The Ideas behind Relativistic Newtonian Dynamics
Distinctions between RN D and GR Dynamics
Testing the RN D and GR Redshift in Strong Gravitation
Terrestrial Tests of the GR and RN D Predictions
Testing the One-Way Speed of Light Predictions
Testing the Relativistic Time Dilation
The Metric of a Field from Several Sources in Whitehead’s and RN D Models
10. Discussion
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