On Tuesday, March 26, 2019 at 5:08:15 PM UTC-6, smitra wrote:
>
> On 26-03-2019 20:29, [email protected] <javascript:> wrote: 
> > On Tuesday, March 26, 2019 at 11:29:08 AM UTC-6, John Clark wrote: 
> > 
> >> On Tue, Mar 26, 2019 at 1:14 PM <[email protected]> wrote: 
> >> 
> >>> _> How do the mathematicians prove it?_ 
> >> 
> >> Mathematicians can't prove that a physical theory is correct, all 
> >> they can do is show that changing the coordinate system (for example 
> >> by rotating the X and Y axis) does not result in different physical 
> >> predictions. Only exparament can tell you if the predictions is 
> >> right, or at least mostly right. 
> >> 
> >> John K Clark 
> > 
> > I'm not asking if GR is correct; rather, whether it is covariant. 
> > Moreover, for SR we can prove covariance, since under the LT, the law 
> > of physics don't change and the SoL is c in any inertial frame. ME are 
> > also invariant under the LT.  AG 
> > 
>
> There are many ways one can do this, the most elegant way is to start 
> with a Lagrangian of a field theory and then demand that it be invariant 
> under general coordinate transforms, which requires factors of the 
> square root of the determinant of the metric tensor to be inserted to 
> compensate for the Jacobian of a coordinate transform. This seemingly 
> rather trivial insertion, will yield the field equations of GR as far as 
> the coupling with the fields desribed by the field theory are concerned. 
>
> Compare this with the way you can derive the Maxwell equations from 
> scratch. You start of a scalar field theory, that is invariant under 
> global gauge transforms phi ---> exp(i alpha) phi. And then you make the 
> constant alpha an arbitrary function of space-time, which destroys the 
> invariance due to derivatives generating additional terms. But you can 
> compensate for these derivatives by including a gauge potential. This 
> then yields the coupling of the scalar field to a new field that we can 
> call the electromagnetic field, and this field will have its own gauge 
> invariant term proportional to the field strength tensor squared. 
>
> So, as Paul Davies puts it, in principle mathematically gifted cave men 
> who had never done any experiments involving electromagnetism and 
> gravity could have deduced the Maxwell equations and the Einstein 
> equations of GR from scratch based only on mathematical elegance. 
>
> Saibal 
>

*As I just told Brent, I think I should spend more time reading relevant 
articles, *
*than asking questions. With that objective, please post some links 
describing *
*the methods you reference above, and the article with Davies quote. TIA, 
AG*

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