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Talk:Counterexamples to Relativity (view source)
Revision as of 22:20, August 2, 2010
, 22:20, August 2, 2010→Curl of the gravitaional field
::::::::: Your definition is too narrow when discussing the theory of relativity, which describes the framework in which the force operates. To be meaningful, the definition must be broader. It must ensure the path independence of the scalar, as well as other scalars independent of that scalar.--[[User:Aschlafly|Andy Schlafly]] 18:12, 2 August 2010 (EDT)
::::::::: Your definition is too narrow when discussing the theory of relativity, which describes the framework in which the force operates. To be meaningful, the definition must be broader. It must ensure the path independence of the scalar, as well as other scalars independent of that scalar.--[[User:Aschlafly|Andy Schlafly]] 18:12, 2 August 2010 (EDT)
:::::::::: Can you tell me what the correct definition is, then? I have pretty good background in this stuff, no need to dumb it down, just be precise. Certainly no field at all is going to conserve every scalar function, so I'd like to know which ones you want. --[[User:KyleT|KyleT]] 18:20, 2 August 2010 (EDT)