What does symmetry of time dilation really mean?

In summary, the symmetry of time dilation refers to the phenomenon in which two observers moving relative to each other each perceive the other's clock as ticking more slowly. This concept arises from the principles of Einstein's theory of relativity, where time is not absolute but relative to the observer's frame of reference. As a result, each observer experiences time differently, leading to the conclusion that time dilation is symmetric; neither observer can claim to be the "correct" one. This symmetry challenges intuitive notions of time and highlights the interconnectedness of space and time in relativistic physics.
  • #1
Chenkel
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Hello everyone,

I've been studying Morin's book and the case for time dilation makes sense, a clock in the rest frame of the moving body counts to ##T_A##, and a clock in the lab frame counts to ##T_B## and we find ##T_B = {\gamma}{T_A}##

What I might be failing to do is understand what the symmetry of time dilation really means.

There is a clock that is not moving, the lab clock, and there is a clock that is moving, the traveling clock, the traveling clock ticks less than the lab clock.

I get this and it makes sense, but why would we say the lab is moving and the traveling clock is the stationary clock for analysis?

In this latter case I see that time dilation is used to explain length contraction of the lab relative to the traveler based on Morins explanation, so maybe that's how time dilation is symmetric?

Maybe if I get good at spacetime diagrams it will make sense.

Looking forward to any help on this matter, thank you.
 
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  • #2
Chenkel said:
a clock in the rest frame of the moving body counts to ##T_A##, and a clock in the lab frame counts to ##T_B## and we find ##T_B = {\gamma}{T_A}##
a clock in the rest frame of the moving body counts to ##\tau_A##, and a pair of synchronized clocks in the lab frame count to ##t_B## and we find ##t_B = {\gamma}{\tau_A}##

Chenkel said:
What I might be failing to do is understand what the symmetry of time dilation really means.
a clock in the rest frame of the lab counts to ##\tau_B##, and a pair of synchronized clocks in the rest frame of the moving body count to ##t_A## and we find ##t_A = {\gamma}{\tau_B}##
 
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  • #3
Chenkel said:
I get this and it makes sense, but why would we say the lab is moving and the traveling clock is the stationary clock for analysis?
Think of a long straight road with mile markers along it. Another straight road crosses the first one at an angle ##\theta##.

On the first road, at the marker one mile after the crossing point, which mile marker on the other road are you level with?

On the second road, at the marker one mile after the crossing point, which mile marker on the other road are you level with?
 
  • #4
Chenkel said:
I get this and it makes sense, but why would we say the lab is moving and the traveling clock is the stationary clock for analysis?
Why not? Why would you assume that a lab, on the rotating surface of the Earth, orbitting the Sun, orbitting the galactic centre, on a collision course towards the Andromeda galaxy is the only valid reference frame in the universe?
 
  • #5
Chenkel said:
What I might be failing to do is understand what the symmetry of time dilation really means.
You keep asking the same question in different threads that you've started. It's actually a very good question, but the answer is subtle.

Since the previous answers involving relativity of simultaneity and spacetime diagrams don't seem to have landed, try focusing on the concept of proper time. Think in terms of events. Let's have two reference frames, ##A## and ##B## moving relative to each other. If two events occur in reference frame ##A## at the same place, then the time that elapses between them is the proper time ##\Delta \tau_A##. Likewise, for two events that occur in the same location in ##B##, the time that elapses between them is ##\Delta \tau_B##.

You seem to be under the impression that time dilation is a relationship between ##\Delta \tau_A## and ##\Delta \tau_B##. It is not!
 
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  • #6
Dale said:
a clock in the rest frame of the moving body counts to ##\tau_A##, and a pair of synchronized clocks in the lab frame count to ##t_B## and we find ##t_B = {\gamma}{\tau_A}##

a clock in the rest frame of the lab counts to ##\tau_B##, and a pair of synchronized clocks in the rest frame of the moving body count to ##t_A## and we find ##t_A = {\gamma}{\tau_B}##
What do you mean by a pair of synchronized clocks?
 
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  • #7
Chenkel said:
What do you mean by a pair of synchronized clocks?
See section 1.3 of Morin's book.
 
  • #8
PeroK said:
See section 1.3 of Morin's book.
I'm aware that loss of simultaneity happens in certain reference frames in the theory.
 
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  • #9
And we're on Thread #4. At least.

You got some good advice in previous threads. It might be a better idea to try and follow this advice than to start a brand new thread where you will likely get the exact same advice.
 
  • #10
Vanadium 50 said:
And we're on Thread #4. At least.

You got some good advice in previous threads. It might be a better idea to try and follow this advice than to start a brand new thread where you will likely get the exact same advice.
Relativity seems like an accepted idea, but time dilation being symmetric and happening in both rest frames seems like it might be contradictory to me. Maybe I just haven't studied enough.
 
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  • #11
Dale said:
a clock in the rest frame of the moving body counts to ##\tau_A##, and a pair of synchronized clocks in the lab frame count to ##t_B## and we find ##t_B = {\gamma}{\tau_A}##

a clock in the rest frame of the lab counts to ##\tau_B##, and a pair of synchronized clocks in the rest frame of the moving body count to ##t_A## and we find ##t_A = {\gamma}{\tau_B}##
So the first paragraph chooses the lab as the rest frame for analysis, and the second paragraph chooses the moving body as the rest frame for analysis?

Why do two different analysis lead to two equations that are inconsistent?
 
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  • #12
Chenkel said:
I'm aware that loss of simultaneity happens in certain reference frames in the theory.
It's not "loss of simultaneity", it's relativity of simultaneity. That means simultaneity is different in every inertial frame, not just "some".

@Vanadium 50 has made a valid point: you keep starting new threads asking the same question. And the answer keeps being the same.

Chenkel said:
Why do two different analysis lead to two equations that are inconsistent?
They don't when you do the analysis correctly. Doing that requires using the full Lorentz transformation equations, which you are not doing. You need to do that. This has already been discussed in your previous threads.
 
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  • #13
Chenkel said:
Relativity seems like an accepted idea, but time dilation being symmetric and happening in both rest frames seems like it might be contradictory to me. Maybe I just haven't studied enough.
For the unpteenth time: You are missing the relativity of simultaneity. You will not understand relativity until you internalize it.
 
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  • #14
Chenkel said:
Why do two different analysis lead to two equations that are inconsistent?
They are not, they are comparing different things.
 
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  • #15
Orodruin said:
They are not, they are comparing different things.
I just don't see how both clocks can think the "other" is ticking slower, seems inconsistent. But I don't know, Albert Einstein is a genius, who am I?
 
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  • #16
Chenkel said:
I just don't see how both clocks can think the "other" is ticking slower, seems inconsistent.
At this point we have done our best to explain it to you. If you still don't get it, the only advice we can give you is to take the time to learn SR from a textbook.

Chenkel said:
But I don't know, Albert Einstein is a genius, who am I?
Someone who does not understand how relativity works the way Einstein did. At this point we can do nothing more to help you fix that, but that's what you need to fix.

This thread is closed.
 
  • #17
Chenkel said:
What do you mean by a pair of synchronized clocks?
I mean two inertial clocks, at rest with respect to each other, that have been synchronized using Einstein’s synchronization convention. This process of synchronizing a set of inertial clocks is the basis of an inertial reference frame.

Chenkel said:
So the first paragraph chooses the lab as the rest frame for analysis, and the second paragraph chooses the moving body as the rest frame for analysis?
Yes.

Chenkel said:
Why do two different analysis lead to two equations that are inconsistent?
They don’t. There is nothing inconsistent with The equations I wrote:
##t_B = {\gamma}{\tau_A}##
##t_A = {\gamma}{\tau_B}##
This is a perfectly consistent set of equations.

You had written
##T_B = {\gamma}{T_A}##
##T_A = {\gamma}{T_B}##
which is inconsistent. But that is not what I wrote.

Chenkel said:
I just don't see how both clocks can think the "other" is ticking slower, seems inconsistent.
That is why I carefully wrote it the way I did. In each frame the two synchronized clocks read more coordinate time than the one clock’s proper time. There is nothing inconsistent about that.

PeterDonis said:
This thread is closed.
Oops, sorry I didn’t notice the closure when I started replying.
 
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FAQ: What does symmetry of time dilation really mean?

What does symmetry of time dilation really mean?

Symmetry of time dilation refers to the fact that time dilation is observed equally by two observers moving relative to each other. If Observer A sees Observer B's clock running slower, Observer B will also see Observer A's clock running slower by the same factor.

How is time dilation symmetric between two observers in relative motion?

Time dilation is symmetric because both observers are in inertial frames of reference, meaning neither is accelerating. According to the theory of relativity, each observer measures the other's time as moving slower due to their relative velocity, making the effect reciprocal.

Why does each observer see the other's clock running slower?

Each observer sees the other's clock running slower due to the relative velocity between them. This effect arises from the Lorentz transformation equations in special relativity, which describe how measurements of time and space change for observers in different inertial frames.

Does symmetry of time dilation violate the principle of relativity?

No, symmetry of time dilation does not violate the principle of relativity. In fact, it is a direct consequence of this principle, which states that the laws of physics are the same in all inertial frames of reference. Neither observer can be considered at absolute rest, so both experience time dilation equally.

Can time dilation symmetry be experimentally verified?

Yes, time dilation symmetry can be experimentally verified. Experiments with particles moving at high speeds, such as muons in particle accelerators, and precise measurements using atomic clocks on fast-moving aircraft or satellites, have confirmed that time dilation is symmetric and consistent with the predictions of special relativity.

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