On Thursday, March 8, 2018 at 7:59:50 PM UTC-5, Brent wrote:
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> On 3/8/2018 4:31 PM, [email protected] <javascript:> wrote:
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> On Thursday, March 8, 2018 at 4:35:35 PM UTC-5, Brent wrote: 
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>> On 3/8/2018 9:48 AM, [email protected] wrote:
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>> On Thursday, March 8, 2018 at 12:36:07 PM UTC-5, Brent wrote: 
>>>
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>>> On 3/8/2018 4:24 AM, [email protected] wrote:
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>>> On Wednesday, March 7, 2018 at 11:04:09 PM UTC-5, Brent wrote: 
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>>>> 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
>>>
>>>
>>> It's not a "resumption" of motion; it's just tilting the direction of 
>>> motion from being along your coordinate time line (which you think of as 
>>> 'not moving') to being along the geodesic (which you think of as 
>>> 'falling').  The 4-momentum of the system, including whatever device you 
>>> were using to keep the particle from falling is conserved.
>>>
>>> Didn't you say you had read Epstein?
>>>
>>> Brent
>>>
>>
>> I said I was reading Epstein. I have it with me while traveling. If 4 
>> momentum is conserved, isn't that the same as saying motion on a geodesic 
>> is postulated? 
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>>
>> No. Motion on a geodesic is force-free motion.  If you have rocket, for 
>> example, you can travel on a non-geodesic, but 4-momentum is still 
>> conserved considering your rocket and its exhaust.
>>
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> *OK, but what I meant was this; when the force causing a non-geodesic 
> motion is discontinued, geodesic motion is restored. Is this baked into the 
> field equations and thus can be understood as the result of the postulates 
> of GR? AG *
>
>
> I wouldn't say "baked in".  You have to represent a particle as 
> concentrated mass point in the equations and then they tell you that, 
> absent other forces, it follows a geodesic.
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>
>> Incidentally, if one accepts GR as a "valid" model of gravity, doesn't 
>> that preclude any coupling between gravity and EM? AG 
>>
>> Photons couple the same as other mass-energy, they travel on geodesics 
>> absent some other interaction.
>>
>
>
> *OK, but what I meant by "coupling" would be if EM had a role in producing 
> the gravitational phenomenon other than its mass-energy contribution. As I 
> understand GR, it is solely the mass-energy of anything that produces the 
> geometry of spacetime, and thus gravity, nothing specifically 
> electromagnetic. AG *
>
>
> Right.  It's any mass-energy.
>
> Brent
>

*This I find troubling. We have two fundamental physical phenomenon, 
gravity and EM, and they seem to have no intrinsic relationship between 
each other. AG *

>
>
>> * Brent*
>>
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