Which clock was slower in special relativity?

In summary, the conversation discusses the twin paradox and the concept of relative motion in the context of special relativity. It is pointed out that motion is relative, but acceleration is not. The difference in the clocks when the twins meet again will be based on which one accelerated. The concept of inertial reference frames is also explained, with the conclusion that both clocks cannot be inertial if they meet more than once.
  • #36
entropy1 said:
But then we get to my point: SR clock differences should be the result of velocity, [...]
Differences are also due to position.

Suppose you are flying from Earth to the moon. I have set up beforehand a clock on the moon and I synchronized it with clocks on Earth. You will of course observe my clock running slow, but you will attribute my thinking that your clocks are running slow to an error I made when I did the synchronization.

(Of course, this situation is perfectly symmetrical. I will observe your clock running slow, but if you synchronized the clocks I would attribute your thinking that my clock is running slow to an error you made when you did the synchronization.)

You have to understand this effect, called the relativity of simultaneity, and how it explains the symmetry of time dilation (that is, how each thinks the other's clocks are running slow).

Once you do that you can start understand the answer to the original question you asked. Of course, you have to understand that the two people involved share the same location twice, and can therefore compare the proper time that elapsed between. I recommend that you learn how to draw spacetime diagrams (it's easy) and see that the clock that took the shorter path through spacetime is the clock that shows the smaller elapsed time.
 
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  • #37
pervect said:
It is convenient to compare clocks using the Einstein synchronization convention

This only works if the clocks are at rest relative to each other. But the OP's question is about clocks that aren't at rest relative to each other. The Einstein synchronization convention does not work for that case.
 
  • #38
PeterDonis said:
This only works if the clocks are at rest relative to each other. But the OP's question is about clocks that aren't at rest relative to each other. The Einstein synchronization convention does not work for that case.

In order to compare the two clocks, one needs a synchronization system. This is a notion of "now". In order to compare the clocks at all, one must pick a frame with an associated clock synchronization mechanism, a notion of "now". It is usual to pick one of the frames in which one the clocks are at rest, but it's also possible to pick a third frame in which neither clock is at rest.

The basic issue that confuses people is that in SR, clock synchronization, the notion of "now", is a frame dependent process in special relativity.
 
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  • #39
pervect said:
The basic issue that confuses people is that in SR, clock synchronization
Also, "how are you synchronising your clocks" is one of those things that sounds like hopeless pedantry when first raised (of course, it's actually critical to understanding relativity). I suspect that's a big part of why it bounces off people's mental filters the first couple of times you mention it.
 
  • #40
pervect said:
In order to compare the two clocks, one needs a synchronization system.

One needs a choice of simultaneity convention. Einstein clock synchronization corresponds to a particular choice of simultaneity convention that works for a pair of clocks that are at rest relative to each other.

You can still choose a simultaneity convention for clocks that are not at rest relative to each other, but that convention won't correspond to Einstein clock synchronization.
 
  • #41
The Einstein conventiion applies to frames of reference, in particular inertial frames of reference, which can be modeled as an infinite array of clocks at rest relative to each other. They fill space-time, so there is a clock present at every possible event. Then these clockss are all synchronized in that frame via the Einstein convention. All the clocks in an inertial frame run at the same rate.

One typically is invited to imagine these "frame clocks" held at a constant distance apart by a rigid structure or framework of some kind.

Using the frame concept, a moving clock can be compared to a co-located "frame" clock. Of course the moving clock will generally be found to run at a different rate than the frame clocks, this is what's called time dilation.

This is all standard SR. GR needs to use more general notions. I tend to use the idea that all that is necessary is to assign unique labels to events. Physically, it is necessary and sufficient to know the unique Lorentz intervals between all sufficiently nearby events to define the space-time geometry.
 
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  • #42
pervect said:
Using the frame concept, a moving clock can be compared to a co-located "frame" clock.
This was, in fact, explicitly done in Einstein's seminal "On The Electrodynamics Of Moving Bodies" paper. It is one of the more confusing aspects of the paper, but it is perfectly legitimate.
 
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  • #43
Dale said:
It is one of the more confusing aspects of the paper, but it is perfectly legitimate.

In §2, Einstein creates also real confusion:
Einstein 1905 said:
Let us furthermore suppose that the two clocks synchronous with the clocks in the system at rest are brought to the ends A and B of a rod, i.e., the indications of the clocks correspond to the "time of the stationary system" at the places where they happen to arrive; these clocks are therefore "synchronous in the stationary system".
...
Therefore the observers moving with the moving rod, thus would not find the clocks synchronous, though the observers in the stationary system would declare the clocks to be synchronous.
Source:
https://en.wikisource.org/wiki/Translation:On_the_Electrodynamics_of_Moving_Bodies#%C2%A7_2._On_the_relativity_of_lengths_and_times%2E

In the commented German version of the paper, the comment says:
comment to Einstein 1905 (translated) said:
The clocks described in the 2nd clause are not only needless, but the experimental set-up is impossible. As Einstein shows consecutively, clocks moving relative to each other tick differently fast. Therefore, the clocks attached to both ends of the moving rod cannot be synchronous with the "rest frame".
 
  • #44
Well, I disagree with the "impossible" comment. It is entirely possible to construct such clocks. In fact, we do something similar with GPS where we simply add a "counter time dilation" factor to the clock frequency. In its rest frame such a clock will not keep correct time, but the goal is specifically to have it keep time in a frame where it is not at rest. It can in fact be done.

I do agree with the "needless" comment. I would even add "unhelpful" or "distracting" or "confusing".
 
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  • #45
Dale said:
Well, I disagree with the "impossible" comment. It is entirely possible to construct such clocks. In fact, we do something similar with GPS where we simply add a "counter time dilation" factor to the clock frequency. In its rest frame such a clock will not keep correct time, but the goal is specifically to have it keep time in a frame where it is not at rest. It can in fact be done.

I do agree with the "needless" comment. I would even add "unhelpful" or "distracting" or "confusing".

For example, it is perfectly possible to to have an arrangement like this, according to an observer at rest with respect to the lower row of clocks:

clock_sync1.gif


But according to an observer at rest with respect to the upper row of clocks, this is what is happening:

clock_snyc2.gif
 
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  • #47
Dale said:
Well, I disagree with the "impossible" comment. It is entirely possible to construct such clocks. In fact, we do something similar with GPS where we simply add a "counter time dilation" factor to the clock frequency.
I'm not sure this is more than a quibble, but if we say a clock is something that measures time, these "clocks" don't qualify in the sense that they don't measure their own proper time. That is perhaps the context in which the "impossible" claim was made.
 
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  • #48
Mister T said:
I'm not sure this is more than a quibble, but if we say a clock is something that measures time, these "clocks" don't qualify in the sense that they don't measure their own proper time.
I don't think that's a quibble - there's a subtlety here about how we measure and use time in our daily lives.

Consider the clocks we use most often: A wall clock synchronized by the 50Hz or 60Hz line voltage signal from the power utility, anything synchronized to a standard time signal broadcast over the air or the internet, the time displayed on airport monitors, anything that shows UTC with or without a timezone offset... None of these are measuring proper time. They are displaying a coordinate time that is never too far off from local proper time and that's what makes them useful to civilization.

Everyone calls these "clocks" but you're right that in the context of a discussion of special relativity, they aren't clocks. That's why finding them called that in Einstein's writing is so confusing. At the turn of the 20th century the distinction between civilization's coordinate time and proper time was not recognized; Einstein of course understood it, but would have no reason not to use the word "clock" as it was generally used then.
 
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  • #49
Mister T said:
I'm not sure this is more than a quibble, but if we say a clock is something that measures time, these "clocks" don't qualify in the sense that they don't measure their own proper time. That is perhaps the context in which the "impossible" claim was made.
Yes, I can see that viewpoint. Certainly that could be.

In any case, you can construct a device that behaves as Einstein described and use it as he described using it. But I can see the viewpoint that would refuse to call that device a clock for the reason you mention.
 
  • #50
I also think it helps a lot to define a clock as a device that measures its proper time in any frame of reference. That doesn't mean that we can't use other measures of time. The GPS is an example that the spacetime structure of GR is the best description we have today. It wouldn't work, if the precise synchronization of the clocks of the satellites and on ground were not considering all relativistic effects.
 

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