The motion is determined by initial conditions. It is not something 
determined by some other physics. 

LC

On Monday, August 3, 2020 at 2:18:07 PM UTC-5 [email protected] wrote:

>
>
> On Monday, August 3, 2020 at 12:15:23 PM UTC-6, Alan Grayson wrote:
>>
>>
>>
>> On Monday, August 3, 2020 at 8:55:17 AM UTC-6, Alan Grayson wrote:
>>>
>>>
>>>
>>> On Sunday, August 2, 2020 at 5:00:22 PM UTC-6, Alan Grayson wrote:
>>>>
>>>>
>>>>
>>>> On Sunday, August 2, 2020 at 1:55:15 PM UTC-6, Lawrence Crowell wrote:
>>>>>
>>>>> I looked at the precession question, wrote it in WORD and then posted 
>>>>> it in the wrong thread. A big line of anti-virus defense is working 
>>>>> off-line. I do a lot of work locally and pop on and off the internet. I 
>>>>> try 
>>>>> to never leave my machines on-line with an open port for anyone or any 
>>>>> bot 
>>>>> to enter to cause mischief.
>>>>>
>>>>> With this the question is odd. How something moves in free and flat 
>>>>> space and spacetime is just determined by its initial conditions.
>>>>>
>>>>> LC
>>>>>
>>>>
>>>> If one starts with SR and zero curvature of spacetime, and places a 
>>>> test particle in that spacetime spatially at rest, how will spacetime tell 
>>>> matter how to move if spacetime isn't curved? AG 
>>>>
>>>
>>> I think in this situation the direction of motion is ambiguous. AG 
>>>
>>
>> No. It doesn't spatially move, but it moves in space-time since the 
>> observer's clock continues to advance. AG 
>>
>
> What bothers me about this is that the spatial coordinates generally 
> depend on each other, and time. In this situation will the geodesic 
> equations yield a solution where the spatial coordinates remain fixed? AG 
>
>>
>>>>>
>>>>>
>>>>>
>>>>> On Sunday, August 2, 2020 at 9:05:57 AM UTC-5 [email protected] 
>>>>> wrote:
>>>>>
>>>>>>
>>>>>>
>>>>>> On Sunday, August 2, 2020 at 5:30:36 AM UTC-6, Lawrence Crowell wrote:
>>>>>>>
>>>>>>> The periapsis or perihelion advance of Mercury is largely a result 
>>>>>>> of classical perturbation theory in classical mechanics. About 10% of 
>>>>>>> the 
>>>>>>> perihelion advance could not be accounted for by perturbation methods 
>>>>>>> in 
>>>>>>> classical mechanics. 
>>>>>>>
>>>>>>> This has to be admired in some ways. Finding the ephemeris of 
>>>>>>> Mercury is tough, for the planet makes brief appearances near the sun 
>>>>>>> in 
>>>>>>> mornings and evenings. Finding an orbital path from its course across 
>>>>>>> the 
>>>>>>> sky is not easy. The second issue is that perturbation methods in 
>>>>>>> classical 
>>>>>>> mechanics are difficult. These were developed arduously in the 19th 
>>>>>>> century 
>>>>>>> and Le Verrier worked on this to find the planet Neptune from the 
>>>>>>> perturbed 
>>>>>>> motion of Uranus in 1848. These methods were worked on through the 19th 
>>>>>>> century. The later work of von Zeipel and Poincare were used to compute 
>>>>>>> the 
>>>>>>> periapsis advance of Mercury, but there was this persistent 
>>>>>>> 43arc-sec/year 
>>>>>>> that resisted these efforts.
>>>>>>>
>>>>>>> It was general relativity that predicted this anomaly in ways that 
>>>>>>> are far simpler than the classical perturbation methods. This 
>>>>>>> post-diction 
>>>>>>> of GR was an initial success in the theory, followed up shortly by the 
>>>>>>> Eddington expedition that found the optical effects of GR in a solar 
>>>>>>> eclipse in 1919.
>>>>>>>
>>>>>>> LC
>>>>>>>
>>>>>>
>>>>>> I appreciate your grasp of the history, but you haven't answered my 
>>>>>> question and don't seem aware of what it is (plus you posted your reply 
>>>>>> on 
>>>>>> the wrong thread). AG 
>>>>>>
>>>>>>>
>>>>>>> On Sunday, August 2, 2020 at 3:49:28 AM UTC-5 [email protected] 
>>>>>>> wrote:
>>>>>>>
>>>>>>>>
>>>>>>>>
>>>>>>>> On Saturday, August 1, 2020 at 10:35:09 PM UTC-6, Alan Grayson 
>>>>>>>> wrote:
>>>>>>>>>
>>>>>>>>> In flat space, which is tantamount to assuming the absence of 
>>>>>>>>> gravity, and non-zero curvature, a body placed at spatial coordinates 
>>>>>>>>> x,y,z, will move because t increments. But if there is zero 
>>>>>>>>> curvature, in 
>>>>>>>>> which direction will it move? That is, how is the direction of motion 
>>>>>>>>> determined? TIA, AG
>>>>>>>>>
>>>>>>>>
>>>>>>>> CORRECTION; above, I meant to write, " ... which is tantamount to 
>>>>>>>> assuming the absence of gravity and ZERO curvature, ... "   AG
>>>>>>>>
>>>>>>>

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