Does the Twin Paradox Break Symmetry in the Zig-Zag Scenario?

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The discussion centers on the Twin Paradox and whether symmetry is broken in various scenarios involving two travelers, A and B, and a companion C. It is established that when B travels to a star and back, the symmetry is broken due to B changing inertial frames while A remains stationary. Both A and B observe each other's clocks differently, with significant time discrepancies resulting from their relative speeds and the effects of light travel time. The conversation also explores how C, traveling with B, perceives time relative to A, leading to further questions about the nature of simultaneity and time dilation. Ultimately, the analysis emphasizes that symmetry is not maintained when one participant changes their frame of reference.
  • #91
This raises me a question. Does TT actually 'see' proper time of HT go backwards as i addressed?
 
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  • #92
ash64449 said:
This raises me a question. Does TT actually 'see' proper time of HT go backwards as i addressed?
I already answered this a couple of times. TT sees HT clock going forward at all times in a zig zag trajectory. That is why TT should find it hard to accept a model that has HT clock going backwards, contrary to what they see.

They see HT clock going slow until first turnaround, then fast until second, then slow again, then fast again. Never backwards. The rate seen is given by the Doppler factor, which is:

√((1+β)/(1-β))

where β = v/c, and v is taken positive if towards (e.g. HT is seen approaching), negative if away.

If you apply this over the different legs, you will find that it correctly shows the final resulting clock comparison.
 
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  • #93
PAllen said:
If you apply this over the different legs, you will find that it correctly shows the final resulting clock comparison.
Yes. For this example Doppler factor is 1/3 for the case when TT moves away from HT and 3 when TT moves towards HT. By using this I can explain Twin Paradox.

When TT reaches planet, His clock will read 6 years and TT will see 2 years as reading in the clock of the HT(with the help of a large telescope). And finally, when TT reaches the earth,6 years have passed, But now TT during these 6 years, TT will see HT's clock moving faster by the factor 3 and hence he will consider 18 years as passed in HT and hence total age of HT is 20 years.

Now for the Peter's Scenario:

When TT reaches planet,6 years passed and TT will see 2 years passed for HT, When TT reaches mid-way,additional 3 years passed and clock runs faster for HT as seen by TT and hence considers 9 years as passed for HT, and again when TT reaches planet,additional 3 year passes and HT clock beats slower as seen by TT and he considers only 1 year as being passed. And finally when TT reaches the earth,TT considers HT's clock to beat additional 18 years.

So total time elapsed for HT as seen by TT is 2+9+1+18=30 years.

Total elapsed proper time for TT is 6+3+3+6=18 years.

So i understand that what is actually seen by TT is accounted by Doppler factor and not frame switch method i was talking about. So my method doesn't actually describe point of view of observer. What is actually seen is correctly explained by Doppler factor-which means time slowing down(Time Dilation) cannot be seen by any observer.

But still Last Answer of my method was correct.
 
  • #94
PAllen said:
Especially given that what you visually see has no such anomaly, nor is there any such anomaly if you are continually exchanging messages with HT.

Yes. When you were talking like this you were talking about the Doppler Factor. I didn't know that.
 
  • #95
ash64449 said:
[..] What is actually seen is correctly explained by Doppler factor-which means time slowing down(Time Dilation) cannot be seen by any observer. [..] .
What is actually seen includes time dilation; I suppose that you used "relativistic Doppler" which includes time dilation, and it's necessary for symmetry of observations between inertial reference systems that are in relative motion. Classical Doppler doesn't include it.
- https://en.wikipedia.org/wiki/Doppler_effect
 
  • #96
harrylin said:
What is actually seen includes time dilation

Yes. It includes Time Dilation .But we don't see Time Dilation.

I can explain Doppler factor PAllen was talking about .I involve only calculation for a single outgoing scenario.

Consider HT send a signal when it's 1 year for him.

Then the signal will reach TT after 4 years which is 5 years of travel for TT in HT's rest frame.

Now using Time Dilation formula, we find only 3 years elapsed for TT.

So TT think 1 year has passed for HT when 3 years is passed for TT. This is what TT 'see'.

If i consider to work in TT's rest frame,only 1.8 years has been passed for HT and not 1 year when 3 years is passed.

Doppler factor includes Time Dilation but we don't see the Effect of Time Dilation. If so, Then TT should have thought 1.8 years passed for HT when 3 years has been passed for TT, But TT see 1 year pass for HT. So we don't see Time Dilation.
 
  • #97
ash64449 said:
What will be the reading of the clocks when TT and HT meet up again according to your scenario according to my analysis?

I don't know because it looks like your analysis is not self-consistent. But we don't need to do the analysis your way to get the answer. There are plenty of other ways to do it.

ash64449 said:
I think If i use HT's rest frame, TT's travel along the space-time is a zig-zag path and by using the relationship between HT's proper time and TT's proper time, i can see what their clocks will read at the end of the scenario.

ash64449 said:
By calculation, I see HT should read 30 years while TT should read 18 years.

Yes, this is one valid way to do it.
 
  • #98
ash64449 said:
Yes. It includes Time Dilation .But we don't see Time Dilation.

I can explain Doppler factor PAllen was talking about .I involve only calculation for a single outgoing scenario.

Consider HT send a signal when it's 1 year for him.

Then the signal will reach TT after 4 years which is 5 years of travel for TT in HT's rest frame.

Now using Time Dilation formula, we find only 3 years elapsed for TT.

So TT think 1 year has passed for HT when 3 years is passed for TT. This is what TT 'see'.

If i consider to work in TT's rest frame,only 1.8 years has been passed for HT and not 1 year when 3 years is passed.

Doppler factor includes Time Dilation but we don't see the Effect of Time Dilation. If so, Then TT should have thought 1.8 years passed for HT when 3 years has been passed for TT, But TT see 1 year pass for HT. So we don't see Time Dilation.
I'm afraid that I can't follow your reasoning, which looks unnecessarily complex to me. A feature of the so-called "twin paradox" is that in the end the clocks are compared side by side, and we can see that the times they display differ considerably. Can you think of a more striking way to "see" time dilation?
 
  • #99
harrylin said:
"see" time dilation

I think Time Dilation means this: When a observer moves relative to us, Time slows down for him relative to us.(not depend on which direction observer moves)

The question that needs to be addressed here is whether we see Time Dilation with our eyes.

The Answer is No. Because We see Relativistic Doppler Effect which include Time Dilation. We 'see' time beats at slower rate for an observer which is moving away from you and we 'see' time run at a faster rate when the observer move towards you. This effect is the one we 'see' which is not Time Dilation. What we see is Relativistic Doppler Effect which includes Time Dilation.

This is the one what i said at the previous post.
 
  • #100
ash64449 said:
I think Time Dilation means this: When a observer moves relative to us, Time slows down for him relative to us.(not depend on which direction observer moves)

The question that needs to be addressed here is whether we see Time Dilation with our eyes.

The Answer is No. Because We see Relativistic Doppler Effect which include Time Dilation. We 'see' time beats at slower rate for an observer which is moving away from you and we 'see' time run at a faster rate when the observer move towards you. This effect is the one we 'see' which is not Time Dilation. What we see is Relativistic Doppler Effect which includes Time Dilation.

This is the one what i said at the previous post.
"Seeing" always includes a certain amount of interpretation of what it is that you think you are seeing. :wink:
 
  • #101
harrylin said:
"Seeing" always includes a certain amount of interpretation of what it is that you think you are seeing. :wink:
What is that interpretation?
 
  • #102
ash64449 said:
What is that interpretation?
Ehm no. Just try to come up with an example of such a thing that you are looking for, and in which you do not interpret! (and compare for example post #7 of this thread).
 
  • #103
ash64449 said:
What we see is Relativistic Doppler Effect which includes Time Dilation.
You may wish to read about "transverse Doppler".
 
  • #104
I think some spacetime diagrams might help to illustrate the two scenarios specified in this thread. The first one comes from post #55:
ash64449 said:
Let the distance between the Earth and planet be 8 light years.(rest length between them)
Let speed of the traveling twin(TT) be 0.8c in both part's of the scenario.
...
In the frame HT uses, TT is moving and hence time runs slower for TT. So HT predicts TT would measure 20*0.6=12 years to reach earth. And hence concludes that in between the events 'TT leaves the earth' and 'TT reaches the earth', proper time elapsed for TT is 12 years and proper time elapsed for HT is 20 years and hence TT is 8 years younger than HT.

HT is shown in blue and elapses 20 years while TT is shown in red and elapses 12 years (the dots mark off 1-year increments of Proper Time for each twin):

TP&Simulataneity1.PNG

The issue of relativistic Doppler was brought up as a way for each twin to observe and keep track of the other ones aging. Here is a diagram showing how HT views TT's aging:

TP&Simulataneity2.PNG

Please note that HT cannot see the progress of TT in real time, he can only see the red signals coming to him from TT at the moment they hit him. But since he knows that he has been inertial the whole time, he can calculate the speed of TT and plot his trajectory as shown in the above diagram based just on what he sees and knows of Special Relativity. But this only works for him because TT starts out coincident with him so he can start integrating TT's speed to determine his distance from him. I did not show the planet in the diagrams but HT would not be able to tell how far away it was simply by looking at the relativistic Doppler coming from it. He could however determine the distance to the planet after he sees TT arrive there.

Similarly, TT can use relativistic Doppler to track the aging of HT and since he presumes that HT remained inertial while he did all the accelerating, he can construct a diagram of the scenario just like HT did:

TP&Simulataneity3.PNG

Another method that was discussed is radar coordinates. In this scheme, each twin continually sends out coded signals earmarked with the time they were sent and later when the echo is received, the received time is averaged with the sent time to establish the time of the measurement and the difference of the received time and the sent time divided by two establishes the distance (assuming units where c=1). Here is a diagram showing just a few of the radar signals sent (in blue) and received (in red) by HT:

TP&Simulataneity4.PNG

You should be able to confirm in the three radar examples that the coordinates that HT calculates match the coordinates in the diagram.

Now let's see what TT does:

TP&Simulataneity5.PNG

I've only shown two radar examples which are enough, plus the start and stop data for TT to construct a diagram but since he is not inertial, it will look different than the one that HT makes or the one he made using relativistic Doppler:

TP&SimulataneityNL6.PNG

This may look like a surprising result but what is significant about this is that it maintains all the same radar and Doppler signals that the previous diagrams enacted. In fact, after TT makes this diagram, he can do the same exercise over again from the point of view of HT and get the inertial reference frame that HT got.

One question that might come up is why would TT bother to use radar coordinates when the relativistic Doppler got him the inertial reference frame more directly. The most important answer is that this method works for distant objects such as the planet. Another answer is that it provides a method to show "the point of view" of a non-inertial observer. However, this particular POV (or any other) does not provide any more information to an observer than an inertial reference frame does but it does provide a mechanism for a non-inertial observer to first construct a non-inertial frame and then convert it to an inertial frame (provided that there is an inertial object that he can take data off of.

In my next post I will show Peter's zig-zag scenario.
 
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  • #105
Finally, we get to Peter's zig-zag scenario:
PeterDonis said:
The scenario I am talking about, which I don't think had been discussed in this thread before I brought it up, would be described using the HT's rest frame as follows: TT leaves and travels outbound to a distant location (planet, space station, whatever); then TT turns around and heads back towards HT; halfway back, TT turns around again and heads back to the planet/space station/whatever; then TT turns around and heads back all the way to HT and they meet up again.
TT can use radar coordinates just like before to construct this diagram but here I show some of the significant radar signals that TT employs:

TP&Simulataneity71.PNG

And from that data he will construct this non-inertial frame:

TP&SimulataneityNL72.PNG
 
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