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| published = 1997
| published = 1997
| journal = [[Galilean Electrodynamics]]
| journal = [[Galilean Electrodynamics]]
| volume = [[8]]
| volume = 8
| number = [[1]]
| number = 1
| pages = 6-7
| pages = 6-7
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==Abstract==
==Abstract==


The orbital precession of the binary pulsar PSR 1913+16 can be related to the quite different precessions of Mercury and other inner planets by one simple formula. Expressed non-dimensionally as degrees of prrecession per degree of orbit, the orbit precession rate is given by 3(M<sub>0</sub>M<sub>a0</sub> / H<sub>tot</sub>)<sup>2</sup> (G/c)<sup>2</sup> . Here M<sub>0</sub> and M<sub>a0</sub> are the masses of the pulsar and its companion, or of the planet and the sun, as the case may be. The H<sub>tot</sub> is the total angular momentum of the system, G is the gravitational constant and c is the speed of light. The formula is obtained by postulating mass increase proportional to the inverse of the distance between bodies.[[Category:Scientific Paper]]
The orbital precession of the binary pulsar PSR 1913+16 can be related to the quite different precessions of Mercury and other inner planets by one simple formula. Expressed non-dimensionally as degrees of prrecession per degree of orbit, the orbit precession rate is given by 3(M<sub>0</sub>M<sub>a0</sub> / H<sub>tot</sub>)<sup>2</sup> (G/c)<sup>2</sup> . Here M<sub>0</sub> and M<sub>a0</sub> are the masses of the pulsar and its companion, or of the planet and the sun, as the case may be. The H<sub>tot</sub> is the total angular momentum of the system, G is the gravitational constant and c is the speed of light. The formula is obtained by postulating mass increase proportional to the inverse of the distance between bodies.


[[Category:Relativity]]
[[Category:Scientific Paper|classical correlation orbital precessions]]
 
[[Category:Relativity|classical correlation orbital precessions]]

Latest revision as of 09:38, 21 July 2026

Scientific Paper
TitleThe Classical Correlation of Orbital Precessions
Author(s)Ernest W Graham
Keywordsgeneral relativity theory, orbit precession
Published1997
JournalGalilean Electrodynamics
Volume8
Number1
Pages6-7

Abstract

The orbital precession of the binary pulsar PSR 1913+16 can be related to the quite different precessions of Mercury and other inner planets by one simple formula. Expressed non-dimensionally as degrees of prrecession per degree of orbit, the orbit precession rate is given by 3(M0Ma0 / Htot)2 (G/c)2 . Here M0 and Ma0 are the masses of the pulsar and its companion, or of the planet and the sun, as the case may be. The Htot is the total angular momentum of the system, G is the gravitational constant and c is the speed of light. The formula is obtained by postulating mass increase proportional to the inverse of the distance between bodies.