Modern physics tends to operate on the idea of geodesics and geometric 
determined flows. A geodesic is "determined" from an initial point, which 
can just be a point where data is specified instead of some point of 
origin, where the position on a manifold and the tangent vector are 
specified. From there the dynamics is completely determined. For a quantum 
system things are more nuanced with there being a bundle of paths with some 
congruent condition given by diffeomorphism and Weyl transformations 
"modded out." 

In spacetime and general relativity these geodesic flows obey the geodesic 
deviation equation dU/ds = R(UV)V, and are determined by the curvature of 
spacetime. Here U = dx/ds is the relative velocity between two test masses. 
Now we might imagine a tether between these two test masses. Now their 
relative separation distance is constant and the two masses are not on a 
geodesic path. However, the center of mass of the two are on a geodesic. 
The individual masses are then on nongeodesic paths due to the material 
forces of the tether.

LC

On Thursday, March 8, 2018 at 6:24:59 AM UTC-6, [email protected] wrote:
>
>
>
> On Wednesday, March 7, 2018 at 11:04:09 PM UTC-5, Brent wrote:
>>
>>
>>
>> On 3/7/2018 5:39 AM, [email protected] wrote:
>>
>> *Thanks for your time and effort, but I don't think you understand my*
>> *question. Suppose a test particle is restrained spatially, say in *
>> *the Sun's gravitational field. When released, it starts to move (toward *
>> *the Sun). How does GR explain this motion? By the advance of time? AG*
>>
>>
>> Time was advancing all along.  Your restraint was a force causing the 
>> particle to follow a non-geodesic path through space-time.  When you 
>> released it, it then followed the "straightest path possible", i.e. a 
>> geodesic.
>>
>> Brent
>>
>
> So time is the "culprit". What has this resumption of spatial motion 
> (along a geodesic in spacetime) have to do with conservation of momentum, 
> if at all ? TIA, AG
>

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