On Thursday, March 8, 2018 at 7:24:59 AM UTC-5, agrays...@gmail.com wrote:
>
>
>
> On Wednesday, March 7, 2018 at 11:04:09 PM UTC-5, Brent wrote:
>>
>>
>>
>> On 3/7/2018 5:39 AM, agrays...@gmail.com 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
>

Or to put the question another way, does it resume geodesic motion due to 
conservation of momentum as Standish alleged, or "because" it is postulated 
by GR, which postulate is incorporated in the field equations? TIA, AG 

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