What Causes Clocks to Appear Unsynchronized in Different Frames of Reference?

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Discussion Overview

This discussion revolves around the synchronization of clocks in different frames of reference, particularly in the context of special relativity. Participants explore the conditions under which synchronized clocks appear unsynchronized to observers in different states of motion, including scenarios involving acceleration and deceleration.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants question under what conditions two synchronized clocks, at rest relative to each other, will appear unsynchronized to an observer who has always been at rest relative to them.
  • There is a discussion about whether the synchronization of clocks by an observer at rest affects their perceived synchronization by another observer who was previously moving.
  • One participant suggests that if the clocks are synchronized by someone at rest relative to them, they will always appear synchronized in an inertial frame that shares the same velocity as the clocks.
  • Another participant introduces the idea that if the clocks are attached to a rigid rod, their synchronization may be affected by the rod's acceleration and Lorentz contraction.
  • Concerns are raised about whether the acceleration and deceleration of the clocks affect their synchronization when returning to an inertial frame.
  • Some participants express uncertainty about the implications of acceleration on the proper time measured by the clocks.
  • There is a suggestion that moving a clock within a moving frame could affect its synchronization with another clock that has remained stationary in that frame.

Areas of Agreement / Disagreement

Participants express differing views on the effects of acceleration and the conditions under which clocks remain synchronized. There is no consensus on the implications of acceleration on synchronization, and the discussion remains unresolved.

Contextual Notes

Participants reference specific scenarios, such as clocks on a rigid rod and the effects of acceleration, which may introduce complexities in understanding synchronization. The discussion highlights the dependence on definitions and assumptions regarding motion and reference frames.

matheinste
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Hello all.

If two clocks are at rest relative to each other and are synchronized using the usual Einstein synch procedure, under what conditions will they appear to be unnsynchronized to another observer who has always been at rest relative to them? Also, if an observer previously moving relative to the synchronized clocks ( and so seeing them out of synch with each other ) accelerates ( decelerates ) to become at rest relative to them, will these same two clocks then appear to be in synch with each other to the previously "moving" observer?

My answers would be that i am unsure of the first part because accelerations would be involved to make any changes, and yes for the second part.

Matheinste.
 
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matheinste said:
If two clocks are at rest relative to each other and are synchronized using the usual Einstein synch procedure, under what conditions will they appear to be unnsynchronized to another observer who has always been at rest relative to them?
Were they synchronized by someone who's at rest relative to them? In that case, "any". Otherwise "none".

matheinste said:
Also, if an observer previously moving relative to the synchronized clocks ( and so seeing them out of synch with each other ) accelerates ( decelerates ) to become at rest relative to them, will these same two clocks then appear to be in synch with each other to the previously "moving" observer?
Yes, assuming that he starts the experiment that attempts to verify that they are in synch after he stops, and finishes it before he starts moving again.
 
Hello Fredrik.

Thanks for your reply.

Yes i should have said that the clocks were synchronized by someone at rest relative to them. I suppose this person could also act as the observer at rest relative to them.

Am i misreading something because you say that in this case the clocks will appear to be UNsynchronized to the observer under any conditions.

The second part is clear.

If the second situation is reversed and the clocks accelerate ( decelerate ) to become at rest relative to an observer who was previously moving relative to them ( and so were out of synch with each other according to him ), will they now appear to him to be in synch with each other. Or does the fact that the sychronized clocks have undergone acceleration affect them.

Matheinste.
 
matheinste said:
Am i misreading something because you say that in this case the clocks will appear to be UNsynchronized to the observer under any conditions.
Oops, I got the alternatives confused somehow. They will always be synchronized in an inertial frame that has the same velocity as the clocks.

If instead they were synchronized by someone who wasn't at rest with respect to the clocks, they will never be synchronized in an inertial frame that has the same velocity as the clocks, unless the velocity (in the clocks' rest frame) of the guy who synchronized them was perpendicular to the line connecting them.

matheinste said:
If the second situation is reversed and the clocks accelerate ( decelerate ) to become at rest relative to an observer who was previously moving relative to them ( and so were out of synch with each other according to him ), will they now appear to him to be in synch with each other. Or does the fact that the sychronized clocks have undergone acceleration affect them.
What a clock measures is the integral of [itex]\sqrt{-dt^2+dx^2}[/itex] along the curve in spacetime that represents its motion, and if I understand your description correctly, the world lines of the two clocks are identical in the observer's rest frame (except for starting position), so the difference between the times they are showing at simultaneous events will not have changed.
 
Thanks Fredrik.

Thats just what i thought.

Matheinste.
 
Hello all.

Just to clear up a specific point which may well have ben covered by previous answers in this thread. I have searched several books but cannot find an answer to this specific point.

Take two clocks in the same inertial reference frame synchronized to each other by an observer in the same frame using the Einstein synch method. If the clocks, along with the obserever are accelerated/decelerated and return to the previous, or another state of inertial motion, will the observer consider them to still be synchronized.

The answers so far in this trhread suggest that they will still be in synch, but i have a feeling that somewhere else i have seen a different answer.

Matheinste.
 
Assuming that the world lines of the two clocks and the world line of this observer guy all look the same in the original rest frame (except for their starting position), the answer is definitely yes. This is an immediate consequence of the definition of proper time and the postulate that clocks measure proper time.

You may have read about the scenario where the clocks are attached to opposite ends of a rigid rod. (It's been discussed in this forum a few times). The rod will be getting shorter (Lorentz contracted) when its speed increases (in the original rest frame). So the rear must be accelerating faster than the front, and later it must be decelerating faster than the front. In this case, the world lines will not be identical.

They might still have the same proper time though, e.g. if the deceleration profile is the "opposite" of the acceleration profile, so that the first half of the world line of the rear is a mirror image of the second half of the world line of the front and vice versa. But they may not have the same proper time in general. (I'm too lazy to check).
 
Hello Frerik.

The attachment to a rigid rod scenario rings a bell. I think that's where i have seen the clocks as being out of synch before, but the case of clocks at either end of an accelerating space ship. I think that answers my question prety well. Thanks again.

Matheinste
 
Fredrik said:
Assuming that the world lines of the two clocks and the world line of this observer guy all look the same in the original rest frame They might still have the same proper time though, e.g. if the deceleration profile is the "opposite" of the acceleration profile, so that the first half of the world line of the rear is a mirror image of the second half of the world line of the front and vice versa. But they may not have the same proper time in general. (I'm too lazy to check).

Maybe I am unclear on what you mean here. Wouldn't the acceleration and deceleration
automatically be reciprocal no matter what the route taken to return to the original frame? How could you get back to the original velocity without exactly equal deceleration.?

My understanding of the asynchronicity effect has been that it is not due to action on the clocks themselves but is associated with the location on the moving frame. Is this incorrect?
Ie: if you move a clock while in motion from the back of the frame to the front wouldn't it then be in synch with a clock that had been there from the beginning? And vice versa.
 
  • #10
Austin0 said:
Wouldn't the acceleration and deceleration automatically be reciprocal no matter what the route taken to return to the original frame? How could you get back to the original velocity without exactly equal deceleration.?
In order to get back to the original velocity, the integral of the acceleration as a function of time over the time interval involved must be zero. If a solid rod that's initially at rest is accelerated for a while and ends up at rest again after a while, then the accelerations of both endpoints will satisfy that condition. I'm just saying that I haven't tried to prove or disprove that this implies that the integral of [itex]\sqrt{dt^2-dx^2}[/itex] along the world line of the front is the same as the integral of [itex]\sqrt{dt^2-dx^2}[/itex] along the world line of the rear.

Austin0 said:
My understanding of the asynchronicity effect has been that it is not due to action on the clocks themselves but is associated with the location on the moving frame. Is this incorrect?
Ie: if you move a clock while in motion from the back of the frame to the front wouldn't it then be in synch with a clock that had been there from the beginning? And vice versa.
As I've been saying, what a clock displays is the integral of [itex]\sqrt{dt^2-dx^2}[/itex] along the curve in Minkowski space that represents its motion (i.e. its "world line"). In the scenario you're describing, the two clocks have very different world lines. dx is =0 everywhere on one of them, but not the other, so the accelerating clock measures a shorter time.
 

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