Time dilation and expansion in accelerated motion

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The discussion centers on two experiments involving time dilation and acceleration in flat space-time. Experiment 1 shows that two identical probes accelerating with constant proper acceleration will record the same duration of acceleration. In Experiment 2, a metal rod is accelerated, raising questions about the proper times recorded by probes at each end, particularly the trailing probe. The concept of rigidity is critical, as a perfectly rigid rod would lead to different proper accelerations at each end due to the relativity of simultaneity, akin to the Bell's Spaceship Paradox. Ultimately, the discussion highlights the complexities of simultaneity and acceleration in special relativity, emphasizing that the behavior of the rod and probes depends on their mechanical properties and the observer's frame of reference.
  • #61
nakurusil said:
This is "Born rigidity". I mentioned it to you. The bar will not undergo any "series of compressions and expansions"

If it is pushed, it will undergo compression.
If it is pulled, it will undergo expansion.
It is all in my post.

Huh! Are you saying "Born rigidity" means that the rod is compressed or stretched, or do I understand you wrongly? It is surely not the accepted definition of "Born rigidity".

Since you are inclined towards keeping it physical, a sudden start to even a moderate lengthwise acceleration will cause some 'ringing' in the length of a rod, although it might only be for a short time before it dampens out.
 
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  • #62
nakurusil said:
...
-if the rod is pushed, it gets compressed (the rear outraces the front)
-if the rod is pulled, it gets extended (the front outraces the rear)
In both cases the clock at the front of the rod and the one at the rear travel at different speeds during the acceleration period, until cruising speed is reached when the force is removed.

Huh! (again). Your post creates the impression that a pulled/pushed rod is stretched/compressed progressively <edit> more and more </edit> in proper length for as long as a constant acceleration lasts. I hope I have read you wrongly!
 
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  • #63
Please drop this Born rigidity nonsense.

The concept of "Born rigidity" has no particular relevance in SR. This is because in all the usual thought experiments inertial stresses are excluded from consideration by (a) assuming sufficiently gentle acceleration and/or (b) assuming any elastic distortion is reversable. The mere reference to a "rigid rod" carries implicit indication that only relativistic effects are under consideration.

My argument on the previous page still stands as valid. I don't think Jorrie has understood that the train must have remained unaffected because the longer and shorter "measured" lengths ( gamma*L & L/gamma) are shown to derive purely from the difference in simultaneity between using synchronised train clocks (longer) or synchronised platform clocks (shorter).

With no reason, effect or cause for any variation in lengths on the train, it follows that the proper acceleration is identical at all points along the train.
As I said, accelerations deduced by platform clock observers, who measure shorter and shorter (L/gamma) lengths at higher velocities, will "seem" to be lower at the front than the rear - but they are not measuring "proper" accelerations !
 
  • #64
I posed "Experiment 3" above to eliminate the vexing rigid rod from the puzzle and see what happens with a purely light-speed connection. This is a realistic problem, since satellites might be coordinated in this way. Does it somehow miss the point of MeJennifer's original question?
 
  • #65
Yes it does miss the point of MeJennifer's problem. In order to maintain constant light pulses, the rear rocket would have to slow its acceleretion, thus falling increasingly behind and yielding entirely different telemetry.
 
  • #66
Jorrie said:
Huh! Are you saying "Born rigidity" means that the rod is compressed or stretched, or do I understand you wrongly? It is surely not the accepted definition of "Born rigidity".

Since you are inclined towards keeping it physical, a sudden start to even a moderate lengthwise acceleration will cause some 'ringing' in the length of a rod, although it might only be for a short time before it dampens out.

Yep. Exactly.
 
  • #67
Diametrically opposing views

Boustrophedon said:
Yes it does miss the point of MeJennifer's problem. In order to maintain constant light pulses, the rear rocket would have to slow its acceleretion, thus falling increasingly behind and yielding entirely different telemetry.

I'm afraid we seem to have diametrically opposing views on this!

I believe that in your train experiment the proper acceleration varies across the length of the "rigid" train, because the proper time varies. During acceleration, clocks in the front will gain time on clocks in the rear, just like the higher clock in the Harvard tower experiment gained time on the lower clock.

On the other hand, in Country Boy's constant period light experiment, I think the proper accelerations will have identical profiles, barring a simple time lag between the front and the rear ship, due to the speed of light.

It is true that the rear ship will fall increasingly farther behind the lead ship, because it started accelerating later and will always have a lower speed. It does not have to slow its proper acceleration relative to the lead ship, as you stated it.

BTW, am I right in feeling that you seem to oppose much of mainstream relativity?
 
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  • #68
Don't jump to conclusions...

Jorrie writes:
I believe that in your train experiment the proper acceleration varies across the length of the "rigid" train, because the proper time varies. During acceleration, clocks in the front will gain time on clocks in the rear

This is a crucial error of reasoning. The forward clock does not "go faster". You are running together two separate things. The clock couldn't "know" how far away the observer is to decide how much faster to go !


What happens is that the clocks continue at the same rate but the shift in simultaneity for rear observers means that they perceive as simultaneous the front clock at a progressively later time ( compared to their own clock ) during acceleration so that it appears to be gaining. Correspondingly the front observer's simultaneity also shifts so that the rear clock appears to be falling behind his own.

Obviously when they re-synchronise clocks either the front clock has to be turned back or the rear clock turned forward or some combination of both.
Since what you like to call the "proper time" is the elapsed period on a standard clock without any readjustment or tampering then the "proper times" are identical and so are the accelerations.

Of course when the've re-synchronised at constant v then the train is as equally valid an inertial system as the platform and can legitimately claim that the platform clocks are unsynchronised with the clocks ahead set forward.
 
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  • #69
Jorrie said:
Huh! (again). Your post creates the impression that a pulled/pushed rod is stretched/compressed progressively <edit> more and more </edit> in proper length for as long as a constant acceleration lasts. I hope I have read you wrongly!

Correct, I have explained this several times. Apparently you have a problem with that and you seem to be in the camp of "alternating compressions / expansions"
 
  • #70
Jorrie said:
Huh! Are you saying "Born rigidity" means that the rod is compressed or stretched, or do I understand you wrongly? It is surely not the accepted definition of "Born rigidity".

Since you are inclined towards keeping it physical, a sudden start to even a moderate lengthwise acceleration will cause some 'ringing' in the length of a rod, although it might only be for a short time before it dampens out.
Forget about how it is named, concentrate on the physics of the problem.
If you apply the force as a step function you will get some ringinging. If you use a different profile (like a ramp) you will get "less" ringing. The point is that ringing disappears after the short transitory regime. What steady effect do you get after the ringing has disapperared ? Compression for pushing and extension for pulling, ok?
It is the difference of the speeds at the two ends of the rod that desynchroizes the clocks for the case of a non-infinitely rigid rod, I thought that you understood and that you agreed with me in an earlier post. This is the problem at hand.
 
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  • #71
Again, as in another thread that was recently locked, this thread seems to be going around in circle, and doing that for a rather lengthy period of time.

I will also re-emphasize that if you wish to argue this based on non-standard physics, then PF is the wrong place to do it, as I'm sure you would have already been aware of since you have read the PF Guidelines very closely and memorized it by heart now. We have let threads like this go on a bit longer than we should simply because we hope that some things can be straightened out. It is obvious that based on how long this thread has gone on, and the number of times things keep going back to the same thing, it isn't going to progress that way.

Therefore, I'm sticking a fork into this one and declare it done. Take note that if a similar thread is started and going along the same trend, it will be deleted without warning and approprate actions against the relevant members will be taken.

Zz.
 
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