> On 19 Apr 2019, at 04:08, [email protected] wrote:
> 
> 
> 
> On Thursday, April 18, 2019 at 6:53:33 PM UTC-6, Brent wrote:
> Sorry, I don't remember what, if anything, I intended to text.
> 
> I'm not expert on how Einstein arrived at his famous field equations.  I know 
> that he insisted on them being tensor equations so that they would have the 
> same form in all coordinate systems.  That may sound like a mathematical 
> technicality, but it is really to ensure that the things in the equation, the 
> tensors, could have a physical interpretation.  He also limited himself to 
> second order differentials, probably as a matter of simplicity.  And he 
> excluded torsion, but I don't know why.  And of course he knew it had to 
> reproduce Newtonian gravity in the weak/slow limit.
> 
> Brent
> 
> Here's a link which might help;
> 
>  https://arxiv.org/pdf/1608.05752.pdf <https://arxiv.org/pdf/1608.05752.pdf>

Yes. That is helpful.

The following (long!) video can also help (well, it did help me)

https://www.youtube.com/watch?v=foRPKAKZWx8 
<https://www.youtube.com/watch?v=foRPKAKZWx8>


Bruno



> 
> AG
> 
> On 4/18/2019 7:59 AM, [email protected] <javascript:> wrote:
>> 
>> 
>> On Wednesday, April 17, 2019 at 7:16:45 PM UTC-6, [email protected] <> 
>> wrote:
>> I see no new text in this message. AG
>>  
>> Brent; if you have time, please reproduce the text you intended. 
>> 
>> I recall reading that before Einstein published his GR paper, he used a 
>> trial and error method to determine the final field equations (as he raced 
>> for the correct ones in competition with Hilbert, who may have arrived at 
>> them first).  So it's hard to imagine a mathematical methodology which 
>> produces them. If you have any articles that attempt to explain how the 
>> field equations are derived, I'd really like to explore this aspect of GR 
>> and get some "satisfaction". I can see how he arrived at some principles, 
>> such as geodesic motion, by applying the Least Action Principle, or how he 
>> might have intuited that matter/energy effects the geometry of spacetime, 
>> but from these principles it's baffling how he arrived at the field 
>> equations. 
>> 
>> AG
>> 
>> 
>> On Wednesday, April 17, 2019 at 7:00:55 PM UTC-6, Brent wrote:
>> 
>> 
>> On 4/17/2019 5:20 PM, [email protected] <> wrote:
>>> 
>>> 
>>> On Wednesday, April 17, 2019 at 5:11:55 PM UTC-6, Brent wrote:
>>> 
>>> 
>>> On 4/17/2019 12:36 PM, [email protected] <> wrote:
>>>> 
>>>> 
>>>> On Wednesday, April 17, 2019 at 1:02:09 PM UTC-6, Brent wrote:
>>>> 
>>>> 
>>>> On 4/17/2019 7:37 AM, [email protected] <> wrote:
>>>>> 
>>>>> 
>>>>> On Tuesday, April 16, 2019 at 9:15:40 PM UTC-6, Brent wrote:
>>>>> 
>>>>> 
>>>>> On 4/16/2019 6:14 PM, [email protected] <> wrote:
>>>>>> 
>>>>>> 
>>>>>> On Tuesday, April 16, 2019 at 6:39:11 PM UTC-6, [email protected] <> 
>>>>>> wrote:
>>>>>> 
>>>>>> 
>>>>>> On Tuesday, April 16, 2019 at 6:10:16 PM UTC-6, Brent wrote:
>>>>>> 
>>>>>> 
>>>>>> On 4/16/2019 11:41 AM, [email protected] <> wrote:
>>>>>>> 
>>>>>>> 
>>>>>>> On Monday, April 15, 2019 at 9:26:59 PM UTC-6, Brent wrote:
>>>>>>> 
>>>>>>> 
>>>>>>> On 4/15/2019 7:14 PM, [email protected] <> wrote:
>>>>>>>> 
>>>>>>>> 
>>>>>>>> On Friday, April 12, 2019 at 5:48:23 AM UTC-6, [email protected] 
>>>>>>>> <>wrote:
>>>>>>>> 
>>>>>>>> 
>>>>>>>> On Thursday, April 11, 2019 at 10:56:08 PM UTC-6, Brent wrote:
>>>>>>>> 
>>>>>>>> 
>>>>>>>> On 4/11/2019 9:33 PM, [email protected] <> wrote:
>>>>>>>>> 
>>>>>>>>> 
>>>>>>>>> On Thursday, April 11, 2019 at 7:12:17 PM UTC-6, Brent wrote:
>>>>>>>>> 
>>>>>>>>> 
>>>>>>>>> On 4/11/2019 4:53 PM, [email protected] <> wrote:
>>>>>>>>>> 
>>>>>>>>>> 
>>>>>>>>>> On Thursday, April 11, 2019 at 4:37:39 PM UTC-6, Brent wrote:
>>>>>>>>>> 
>>>>>>>>>> 
>>>>>>>>>> On 4/11/2019 1:58 PM, [email protected] <> wrote:
>>>>>>>>>>>> 
>>>>>>>>>>>> 
>>>>>>>>>>>> He might have been referring to a transformation to a tangent 
>>>>>>>>>>>> space where the metric tensor is diagonalized and its derivative 
>>>>>>>>>>>> at that point in spacetime is zero. Does this make any sense?
>>>>>>>>>>> 
>>>>>>>>>>> Sort of. 
>>>>>>>>>>> 
>>>>>>>>>>> 
>>>>>>>>>>> Yeah, that's what he's doing. He's assuming a given coordinate 
>>>>>>>>>>> system and some arbitrary point in a non-empty spacetime. So 
>>>>>>>>>>> spacetime has a non zero curvature and the derivative of the metric 
>>>>>>>>>>> tensor is generally non-zero at that arbitrary point, however small 
>>>>>>>>>>> we assume the region around that point. But applying the EEP, we 
>>>>>>>>>>> can transform to the tangent space at that point to diagonalize     
>>>>>>>>>>>                                                       the metric 
>>>>>>>>>>> tensor and have its derivative as zero at that point. Does THIS 
>>>>>>>>>>> make sense? AG
>>>>>>>>>> 
>>>>>>>>>> Yep.  That's pretty much the defining characteristic of a Riemannian 
>>>>>>>>>> space.
>>>>>>>>>> 
>>>>>>>>>> Brent
>>>>>>>>>> 
>>>>>>>>>> But isn't it weird that changing labels on spacetime points by 
>>>>>>>>>> transforming coordinates has the result of putting the test particle 
>>>>>>>>>> in local free fall, when it wasn't prior to the transformation? AG 
>>>>>>>>>> 
>>>>>>>>> It doesn't put it in free-fall.  If the particle has EM forces on it, 
>>>>>>>>> it will deviate from the geodesic in the tangent space coordinates.   
>>>>>>>>>                                                          The 
>>>>>>>>> transformation is just adapting the coordinates to the local 
>>>>>>>>> free-fall which removes gravity as a force...but not other forces.
>>>>>>>>> 
>>>>>>>>> Brent
>>>>>>>>> 
>>>>>>>>> In both cases, with and without non-gravitational forces acting on 
>>>>>>>>> test particle, I assume the trajectory appears identical to an 
>>>>>>>>> external observer, before and after coordinate transformation to the 
>>>>>>>>> tangent plane at some point; all that's changed are the labels of 
>>>>>>>>> spacetime points. If this is true, it's still hard to see why 
>>>>>>>>> changing labels can remove the gravitational forces. And what does 
>>>>>>>>> this buy us? AG
>>>>>>>> 
>>>>>>>> You're looking at it the wrong way around.  There never were any 
>>>>>>>> gravitational forces, just your choice of coordinate system made 
>>>>>>>> fictitious forces appear; just like when you use a merry-go-round as 
>>>>>>>> your reference frame you get coriolis forces. 
>>>>>>>> 
>>>>>>>> If gravity is a fictitious force produced by the choice of coordinate 
>>>>>>>> system, in its absence (due to a change in coordinate system) how does 
>>>>>>>> GR explain motion? Test particles move on geodesics in the absence of 
>>>>>>>> non-gravitational forces, but why do they move at all? AG
>>>>>>>> 
>>>>>>>> Maybe GR assumes motion but doesn't explain it. AG 
>>>>>>> 
>>>>>>> The sciences do not try to explain, they hardly even try to  interpret, 
>>>>>>> they mainly make models. By a model is meant a  mathematical construct 
>>>>>>> which, with the addition of certain verbal  interpretations, describes 
>>>>>>> observed phenomena. The justification of  such a mathematical construct 
>>>>>>> is solely and precisely that it is  expected to work.
>>>>>>>     --—John von Neumann
>>>>>>> 
>>>>>>>> 
>>>>>>>> Another problem is the inconsistency of the fictitious gravitational 
>>>>>>>> force, and how the other forces function; EM, Strong, and Weak, which 
>>>>>>>> apparently can't be removed by changes in coordinates systems. AG
>>>>>>>> 
>>>>>>>> It's said that consistency is the hobgoblin of small minds. I am 
>>>>>>>> merely pointing out the inconsistency of the gravitational force with 
>>>>>>>> the other forces. Maybe gravity is just different. AG 
>>>>>>> 
>>>>>>> That's one possibility, e.g entropic gravity.
>>>>>>> 
> 
> 
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