On Wednesday, October 1, 2025 at 11:52:40 PM UTC-6 Alan Grayson wrote:

On Wednesday, October 1, 2025 at 10:41:33 PM UTC-6 Brent Meeker wrote:



On 10/1/2025 6:09 PM, Alan Grayson wrote:



On Wednesday, October 1, 2025 at 6:11:55 PM UTC-6 Brent Meeker wrote:



On 10/1/2025 6:38 AM, Alan Grayson wrote:



On Wednesday, October 1, 2025 at 7:20:13 AM UTC-6 John Clark wrote:

On Wed, Oct 1, 2025 at 8:29 AM Alan Grayson <[email protected]> wrote:

*> Have physicists in the last 120 years claimed that two paths of 
different lengths in spacetime which start and end at same events, have the 
same accelerations, except Brent in his diagram? AG*


*In a word, yes. Two worldlines between the same events in spacetime can 
have different lengths even if both involve acceleration. And proper time 
is the length of your world line. But of course if they have identical 
acceleration histories then they are in the same worldline, not a different 
one.*


You're writing nonsense. Brent has two worldlines with different lengths, 
claiming they have identical accelerations. AG 

And he included diagrams showing the accelerations had the same amplitudes 
and durations.  And that even was redundant.  From the diagram it is clear 
that Red and Blue had the same velocity at the initiation of their 
accelerations and they turned their velocity thru the same angle in each 
period of acceleration...hence one can infer mathematically that their 
(acceleration*duration) products were the same.

Brent


*That was your intention, and it appears so. But since the longer path goes 
further out, away from the shorter path, I don't think splitting the 
necessary accelerations into two parts implies the summed accelerations are 
the same as the acceleration for the shorter path. As I previously stated, 
the standard TP problem, with one twin spatially fixed and other traveling, 
is a limiting case of your diagram, and in that case the accelerations are 
not equal. AG*

The accelerations in my diagram are four equal changes in velocity.  I 
split the turnaround into two burns for Red to make it clear that they were 
the same delta-v and for Blue's two, as shown at the left. 

 

You keep bringing up you "standard TP" problem, but by my examples I've 
shown that every proposed explanation (e.g. they experience different 
accelerations is you latest) is nullified by one or more example (like this 
one).  If it can't be due to acceleration in this example, or in the 
gravitational slingshot example, or in the triplet example, why would you 
continue to suppose it could be due to acceleration in your "standard" 
example.


*You're trying to show that the difference in clock rates depends only on 
spacetime length. What I am suspecting, is that in this particular case, 
the clock rates are different, but your claim that the accelerations are 
identical, is flawed. I do that by examining two limiting cases, which I 
acknowledsge isn't a proof, but only a suggestion. AG  *


*Looking further into this particular scenario, I think you've created a 
specific geometry which demonstrates the two paths have the same 
accelerations, and since the elapsed time along each path is different, it 
can't depend on acceleration. However, there are other paths wherein the 
accelerations won't be equal, where the endpoints are identical. So, if you 
want to generally show that the differential elapsed clock time just 
depends on path length, you can dispense with your diagrams entirely, and 
instead prove that in spacetime everything moves at light speed, and thus 
when comparing paths, one need only integrate the velocity along a path, 
and that will be sufficient to show that when comparing several paths, even 
those whose endpoints are not juxtaposed, that the longest path produces 
the shortest elapsed time. If you're so damned smart that you can easily 
put me down, how come you haven't thought of this solution, which allows 
you to totally dispense with your diagrams, and do a general solution, to 
prove that elapsed time depends only path length, and the longer the path 
length, the shorter the elapsed time, compared to other paths, even those 
whose endpoints are not juxtaposed? AG*

*Concerning your solution using GR, where the turnaround is due to some 
gravitating body, you claimed that the acceleration is zero since the clock 
is in free fall. I recall you used the formula F=ma, plugging F=0 and 
concluding a=0, where F=0 comes from Einstein's "happy thought" that 
gravity isn't a force. I don't like this line of reasoning because you're 
conflating GR with Newtonian Mechanics. The mystery I'd like you to 
address, if you can, is how gravitational acceleration can be non-zero -- 
which it is, assuming we're not changing our definition of acceleration -- 
in the absence of any gravitational force? TY, AG*

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