On Monday, December 18, 2017 at 8:36:29 PM UTC, Brent wrote:
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> On 12/17/2017 2:39 PM, [email protected] <javascript:> wrote:
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> On Sunday, December 17, 2017 at 12:21:27 AM UTC, Brent wrote: 
>>
>>
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>> On 12/16/2017 2:59 PM, [email protected] wrote:
>>
>> There's a problem applying SR in this situation because neither the 
>> ground or orbiting clock is an inertial frame.AG
>>
>>
>> An orbiting clock is in an inertial frame.  An inertial frame is just one 
>> in which no forces are acting (and gravity is not a force) so that it moves 
>> with constant momentum along a geodesic.  Although it's convenient for 
>> engineering calculations, from a fundamental veiwpoint there is no separate 
>> special relativity and general relativity and no separate clock 
>> corrections.  General relativity is just special relativity in curved 
>> spacetime.  So clocks measure the 4-space interval along their path - 
>> whether that path is geodesic (i.e. inertial) or accelerated.
>>
>
> *Interesting way to look at it. So free falling in a gravity field is an 
> extension of SR. But the thing I find puzzling is that in GR the curvature 
> of space-time is caused by the presence of mass, yet I can draw the path of 
> an accelerated body as necessarily a curve in a space-time diagram. I am 
> having trouble resolving these different sources of curvature. AG*
>
>
> An accelerated body, i.e. one a force is acting on (a rocket, you standing 
> on the ground) is following a curved path that is more curved than the 
> "straightest" path.  I put "straightest" in scare quotes because in the 
> curved spacetime the "straight" path is a geodesic which is still 
> curved...it's just the straightest possible path in the given spacetime.  
>
> It is not true that "I can draw the path of an accelerated body as 
> necessarily a curve in a space-time diagram". 
>



*I was referring to flat space-time, for example as a two dimensional 
representation using x and t coordinates. If one models an accelerating 
particle, it necessarily moves on a curved path. So I think this is very 
suggestive; that one can substitute acceleration for space-time curvature 
induced by gravity or mass-energy, insofar as gravity produces an 
acceleration field. AG *

> In general, if you drew a straight line in some coordinate representation 
> of a curved spacetime, it would correspond to an accelerated (non-geodesic) 
> path.  Imagine drawing a straight line past the Earth.  It would take 
> thrust to fly a rocket along that path.  Of course you could construct a 
> coordinate system around the Earth such that straight lines on the diagram 
> corresponded to geodesics, but it would be a very messy and distorted 
> coordinate system.  
>   
> Brent
>

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