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Talk:Theory of relativity (view source)
Revision as of 19:37, April 15, 2012
, 19:37, April 15, 2012→Newtonian explanation of Mercury's precession
The issue here is not whether the exponent is precisely two or not but that you have to have a model which explains all (or at least as many as possible) observations. To get the precision of Mercury right you produce a model which then fails to explain the observed precession of every other body in the solar system. This seems to be a good experimental demonstration that Newcomb-Hall is wrong (or least inadequate as a model). [[User:Jloveday|Jloveday]] 15:32, 15 April 2012 (EDT)
The issue here is not whether the exponent is precisely two or not but that you have to have a model which explains all (or at least as many as possible) observations. To get the precision of Mercury right you produce a model which then fails to explain the observed precession of every other body in the solar system. This seems to be a good experimental demonstration that Newcomb-Hall is wrong (or least inadequate as a model). [[User:Jloveday|Jloveday]] 15:32, 15 April 2012 (EDT)
== First sentence of article contradicted by the rest ==
Given that main body of the article now largely deals with the things GR can explain (including the precession of Mercury) should not the first sentance be changed?[[User:Jloveday|Jloveday]] 15:37, 15 April 2012 (EDT)