On Thursday, March 8, 2018 at 6:36:36 PM UTC-6, [email protected] wrote:
>
>
>
> 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 *
>

The flow can be a path in a space with a Euclidean metric. On leaving JFK 
for Heathrow you fly pretty close to Iceland. It is just a minimal path on 
a sphere. That is another example. Time has not that much to do with it 
other than in the Lorentzian metric there is the light cone structure and 
hyperbolic transformations.

LC
 

>
> 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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