On Thursday, March 8, 2018 at 2:52:11 PM UTC-5, Lawrence Crowell wrote:
>
> Modern physics tends to operate on the idea of geodesics and geometric 
> determined flows. 
>

*Do you agree that the fact that the flow is geodesic is ultimately a 
postulate, and the existence of the flow is rooted in the monotonic 
increase of time? AG *

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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