What Causes the Twins Paradox and Length Contraction in Relativity?

  • #51
I don't know. I can't follow what you've written and I'm not going to finish your calculations.

The answers are

red worldline ##\tau = \sqrt{(14.54)^2 - (3.64)^2} = 14.08 ##
other worldline ##\tau = \sqrt{(14.54)^2 - (8-3.64)^2} = 13.87##

stationary worldline ##\tau = 14.54##

I'm hoping you might grasp some of the princples of relativity from this exercise.

You have made spacetime diagram, and calculated some proper times, so it could be progress.

Can you work out the time on the blue worldline when a light beam from the origin hits it ?
 
  • Like
Likes Stephanus
Physics news on Phys.org
  • #52
Mentz114 said:
I don't know. I can't follow what you've written and I'm not going to finish your calculations.
The answers are
red worldline ##\tau = \sqrt{(14.54)^2 - (3.64)^2} = 14.08 ##
other worldline ##\tau = \sqrt{(14.54)^2 - (8-3.64)^2} = 13.87##
stationary worldline ##\tau = 14.54##
Yes, the our calculations matches. Now I'm using calculator.

Mentz114 said:
Can you work out the time on the blue worldline when a light beam from the origin hits it ?
Wait...
 
  • #53
Mentz114 said:
Can you work out the time on the blue worldline when a light beam from the origin hits it ?
Hits it.
Hits who? Blue worldline?
##\sqrt{14.54^{2} - (8-3.64)^2}##?
13.87 you mean?
The lights hits Blue when his clocks is 13.87?
 
  • #54
No, it's not that way.
The light hits blue world line I think is an intersection
Between blue and the vertical line.
A perpendicular line from blue to vertical line. Is that so?
 
  • #55
No, not perpendicular. But 450 from vertical lines. That's how x = t
Tell me. Which one?
 
  • #56
Stephanus said:
No, not perpendicular. But 450 from vertical lines. That's how x = t
Tell me. Which one?

This one. The WL of the light is as you say ##x=t## and the thing is on ##x=8-vt## so you can get the intersection on the appraoching WL.

Then make a triangle and work out a ##t^2-x^2## and you got it.
 
  • #57
I think the latter, let me calculate.
for x = t from the origin, so...
##t = x - \frac{2}{0.55}## this is 450 from origin
##0.3t = 8-x## this is b velocity
They will meet at...
##1.3x - \frac{0.6}{0.55} - 8 = 0##
##x ≈ 7##
##t = \frac{1.85}{0.55} = 3.36##
The signal from the origin hits B at (7,3.36)
 
  • #58
Mentz114 said:
This one. The WL of the light is as you say ##x=t## and the thing is on ##x=8-vt## so you can get the intersection on the appraoching WL.

Then make a triangle and work out a ##t^2-x^2## and you got it.
Thanks. But I already calculated before your alert popped up. Is it time dilation in PF forum?
Thanks a lot Mentz, I have to go to sleep. It's 02:00 AM in the morning here.
Why time runs faster when I chat with you? Hmmhh... It's the relativity I think. Don't realize it's already 2:00AM.
Shall we continue tomorrow? Or today noon
Thanks, bye.
 
  • #59
Solving ##x=t## with ##x=8-vt## gets ##t=8-vt## so ##t=8/(1+v)=6.15##
and ##x=6.15##.

I'm sorry to keep you awake.
 
  • #60
Mentz114 said:
Solving ##x=t## with ##x=8-vt## gets ##t=8-vt## so ##t=8/(1+v)=6.15##
and ##x=6.15##.

I'm sorry to keep you awake.
No, no, no. Don't be sorry. I liked that.
It helps me much.
 
  • #61
Mentz114 said:
Solving ##x=t## with ##x=8-vt## gets ##t=8-vt## so ##t=8/(1+v)=6.15##
and ##x=6.15##.

I'm sorry to keep you awake.
If by origin you mean (0,0), then ##8/1.3 = 6.15##
I tought it's from D (3.36,0) Point D in your graph.
 
  • #62
Stephanus said:
If by origin you mean (0,0), then ##8/1.3 = 6.15##
I tought it's from D (3.36,0) Point D in your graph.

I drew the light ray on the graph. It is thin yellow line.
 

Attachments

  • pf-st-3.png
    pf-st-3.png
    13.5 KB · Views: 414
  • Like
Likes Stephanus
  • #63
Mentz114 said:
I drew the light ray on the graph. It is thin yellow line.
The light that comes from the origin.

If this is a Spacetime diagram. And C is the centre.
Is it true, that C were/will never be in magenta area? Not even in 450 lines?
Is it true, that C could be in the cyan area below?
 

Attachments

  • SpaceTime.jpg
    SpaceTime.jpg
    16.1 KB · Views: 423
  • #64
Events can exist at every point on the diagram. An event is a pair of numbers (t,x).
 
  • #65
But, for events to happen at the magenta region, that events should travel x>t?
I mean travel faster than light from c point of view?
But I think, I know why there is Twins Paradox.
It is simultaneity of events which responsible, is it so?
 
  • #66
Events can exist anywhere, and they don't "travel". Things that are traveling appear as sloped lines in your graph. Events are points on your graph. More physically an event is something like turning on your rockets. That happens at a point in space at an instant in time, which can't be said to be moving.

That said, you are correct that events in the magenta region cannot be reached from the origin without exceeding the speed of light. An example would be a car crash in London and a simultaneous (in some frame) car crash in New York. If one was at the origin the other was in the magenta region.
 
  • Like
Likes Stephanus
  • #67
Ibix said:
Events can exist anywhere, and they don't "travel". Things that are traveling appear as sloped lines in your graph. Events are points on your graph. More physically an event is something like turning on your rockets. That happens at a point in space at an instant in time, which can't be said to be moving.

That said, you are correct that events in the magenta region cannot be reached from the origin without exceeding the speed of light. An example would be a car crash in London and a simultaneous (in some frame) car crash in New York. If one was at the origin the other was in the magenta region.
Back again to Twins Paradox.
Supposed there's a Type 1a Supernova, 1000 lys away. We know that it's 1000 lys because of its brightness. And suddenly it moves toward us at 0.1 c.
What would we see? Nothing changes, is this right?
Suddenly, 1000 years later, we'll see that the star is blue shifted toward us or at least it changes. Is this right? And keeps getting bigger and bigger. And also 1000 years later we'll experience that time in the supernova runs faster
I know, I know, supernova only lasts a few weeks or years.

Now, what if WE move toward the supernova. We'll see it blue shifted right away. Is this right? We'll experience doppler effect right away and we'll experience that time in the supernova runs faster.

In both cases, we'll experience that times slows for us, but at different date. Time dilation and length contraction work both ways.
But if we move, we'll experience those effect RIGHT AWAY.
But if we at the 'rest frame' and the other object is moving toward us. We'll notice that time/length,etc from that object also dilated/contracted WHEN the object's WORLDLINE reaches us?
Is that so?
Is that why there's Twins Paradox? Simultaneity of events?
 
  • #68
Stephanus said:
Back again to Twins Paradox.
Supposed there's a Type 1a Supernova, 1000 lys away. We know that it's 1000 lys because of its brightness. And suddenly it moves toward us at 0.1 c.
What would we see? Nothing changes, is this right?
Correct. Although I'm not sure how you intend to accelerate a supernova to 0.1c.
Stephanus said:
Suddenly, 1000 years later, we'll see that the star is blue shifted toward us or at least it changes. Is this right? And keeps getting bigger and bigger.
The supernova would be blue-shifted, yes. You don't need to say "towards us" in this context.
Stephanus said:
And also 1000 years later we'll experience that time in the supernova runs faster
I know, I know, supernova only lasts a few weeks or years.
Not really. We will see the supernova evolving rapidly due to the decreasing lightspeed delay. But if we correct for the changing delay we will find that the supernova is evolving more slowly than a non-moving supernova, and this is due to time dilation.
Stephanus said:
Now, what if WE move toward the supernova. We'll see it blue shifted right away. Is this right? We'll experience doppler effect right away and we'll experience that time in the supernova runs faster.
Yes, although again there is an effect from changing light travel time and an effect from time dilation. So we would, again, see that the supernova was running fast, but could subtract out the light travel time and deduce that time was running slow at the supernova.
Stephanus said:
In both cases, we'll experience that times slows for us, but at different date. Time dilation and length contraction work both ways.
But if we move, we'll experience those effect RIGHT AWAY.
We will always experience time for us at one second per second. That's more or less what time is.
Stephanus said:
But if we at the 'rest frame' and the other object is moving toward us. We'll notice that time/length,etc from that object also dilated/contracted WHEN the object's WORLDLINE reaches us?
Is that so?
No. When an object's worldline reaches you, it has crashed into you. When an event's light cone reaches you, it is possible to see that event. You can't see it before because the light didn't have time to reach you yet.
Stephanus said:
Is that why there's Twins Paradox? Simultaneity of events?
You aren't really talking about simultaneity here. You are talking about when people perceive events, which is a separate topic.

The reason for differential aging in the twin paradox is that the twins take different "length" routes through space-time. The point (or a point, anyway) of the twin paradox is to show that you must always take relativity of simultaneity into account, and if you don't you will get silly answers.

Let me ask you a question. I drive from A to B in a straight line, and my odometer reads 100 miles. You take a triangular route from A to B via C, and your odometer reads 120 miles. But we started in the same place and finished in the same place. How would you explain the difference in our odometer readings to me?
 
  • Like
Likes Stephanus
  • #69
Ibix said:
Correct. Although I'm not sure how you intend to accelerate a supernova to 0.1c.
Come on..., I was just trying to say that even though an object moves toward us, we'll never know if it HAS MOVED toward us until it worldline "crashes" us. Or I should have said, if it's a probe with laser signal emitted to us, we'll never know that the probe is moving toward us, until the last signal emitted when the probe still at rest reaches us. But if we move toward the supernova/probe, we'll realize at once that that thing is getting closer. Especially a type 1a supernova, as you certainly know it's a standard candle.
Ibix said:
The supernova would be blue-shifted, yes. You don't need to say "towards us" in this context.
Yes, yes. Thanks. It greatly improves my logic. Thank you. We could have flown away from Andromeda 100 km/s, still its light is blueshifted.

Ibix said:
Let me ask you a question. I drive from A to B in a straight line, and my odometer reads 100 miles. You take a triangular route from A to B via C, and your odometer reads 120 miles. But we started in the same place and finished in the same place. How would you explain the difference in our odometer readings to me?
You're taking the hypotenuse route.
To calculate the angle you take, we should have used ##asin(\frac{100}{120})##.
And of course in space time. The hypotenuse should be...
##\sqrt{100^2-\sqrt{120^2-100^2}^2} = \sqrt{20000-14400} = \frac{\sqrt{140}}{20}##
 
Last edited:
  • #70
And even though MOTION IS RELATIVE and length contraction and time dilation is MUTUAL, in Supernova case, if we move toward the supernova, we'll know AT ONCE that the distance between the supernova and us is receding. But if the supernova moves toward us, we'll have to WAIT till its wordline reaches us, so we know that the distance is receding.
I think there are two cases here.
A. We move toward the supernova.
Time dilation and length contraction effect only experienced by us. The supernova doesn't "experience" time dilation and length contraction.
Time dilation here is, if somehow there's clock or signal from the supernova traveling toward us, we'll see that the clock in the supernova is faster and somehow the supernova will looks oblate not sphere, in short we'll see that the supernova is length contracted.
B. The supernova moves toward us.
We'll never know that it has alread moved toward us. And once its worldline reaches us, then we'll see that its clock is faster and its length is contracted. Of course an observer in the neutron star/black hole/supernova ignoring the strong gravity, will see that our clock is mutually faster and our length is contracted.
 
  • #71
Stephanus said:
I was just trying to say that even though an object moves toward us, we'll never know if it HAS MOVED toward us until it worldline "crashes" us.
No - we'll know when the event's light cone intersects our worldline. In other words, when the light from the supernova reaches us.
Stephanus said:
You're taking the hypotenuse route.
To calculate the angle you take, we should have used ##asin(\frac{100}{120})##.
And of course in space time. The hypotenuse should be...
##\sqrt{100^2-\sqrt{120^2-100^2}^2} = \sqrt{20000-14400} = \frac{\sqrt{140}}{20}##
But if you're happy with "the route is shorter because I took the hypotenuse", why aren't you happy with "one twin's time is longer because he took the direct route"?

Stephanus said:
And even though MOTION IS RELATIVE and length contraction and time dilation is MUTUAL, in Supernova case, if we move toward the supernova, we'll know AT ONCE that the distance between the supernova and us is receding. But if the supernova moves toward us, we'll have to WAIT till its wordline reaches us, so we know that the distance is receding.
But an observer near the supernova (if he can accelerate it to 0.1c, he can avoid being destroyed by it), would know it had started moving immediately, while he wouldn't know we had started moving for 1000 years. The situation is completely symmetrical.
Stephanus said:
I think there are two cases here.
A. We move toward the supernova.
Time dilation and length contraction effect only experienced by us. The supernova doesn't "experience" time dilation and length contraction.
Time dilation here is, if somehow there's clock or signal from the supernova traveling toward us, we'll see that the clock in the supernova is faster and somehow the supernova will looks oblate not sphere, in short we'll see that the supernova is length contracted.
No one ever experiences time dilation or length contraction. It's always something that one measures in someone else. So, to you, the supernova's clocks will be ticking slowly and it will appear length contracted (in the direction pointing towards us, so careful measurement will be needed). To an observer on the supernova, they are at rest and you are in motion, so it is your clocks that are running slow and you who will be length contracted in the direction of motion.
Stephanus said:
B. The supernova moves toward us.
We'll never know that it has alread moved toward us. And once its worldline reaches us, then we'll see that its clock is faster and its length is contracted. Of course an observer in the neutron star/black hole/supernova ignoring the strong gravity, will see that our clock is mutually faster and our length is contracted.
No one ever experiences time dilation or length contraction. It's always something that one measures in someone else. So, to you, the supernova's clocks will be ticking slowly and it will appear length contracted (in the direction pointing towards us, so careful measurement will be needed). To an observer on the supernova, they are at rest and you are in motion, so it is your clocks that are running slow and you who will be length contracted in the direction of motion.

There's a reason those two paragraphs are identical: your two scenarios are identical except for who accelerates. You can tell if it was you who accelerated because you'll have felt the force. If you were somehow incapacitated during the acceleration phase, you have no way to know if it was you who accelerated just now, or the supernova that accelerated 1000 years ago.

None of the above is relevant to the twin paradox.

The space-time diagrams you've been drawing with Mentz are effectively maps of space-time, showing where and when things happen and tracing out how they move. The Lorentz transforms relate the map drawn by one person to the map drawn by another in relative motion. All the stuff about length contraction and time dilation and the relativity of simultaneity and differential aging is there.

All the stuff about light travel time is an additional layer of complexity on top of that. I strongly advise you not to worry about it until you've got the maps sorted out. Make sure you understand the terrain on Google Maps before you switch to Street View, or you'll just get lost.

Yes, we cannot know the supernova has started moving until it's light reaches us. That does not stop us from, after the fact, drawing a map of what must have happened. Here is a pair of space-time diagrams showing us in blue and the supernova in red. I have added dots every 500 years on each worldline.
sn_minkowski.png

In the left-hand diagram, the supernova is in motion and we are at rest. Note that the red dots are slightly wider spaced than the blue ones because of time dilation - there are 20 red dots and 21 blue dots. In the right-hand diagram, we are in motion and the supernova is at rest. In this frame our clocks are time-dilated, but we started them early - so there are still 20 red dots and 21 blue dots.

I haven't drawn on any light pulses because they aren't necessary to understand what's going on with the clocks. I repeat that I would advise not worrying about them - I think you are confusing yourself by trying to sort out the details of what we would see without having a grasp of the big picture.
 
  • Like
Likes Stephanus and Mentz114
  • #72
Thanks Ibix for your answer.
Mentz114 has really helped me understanding Space time diagram, at least I know about that.
Ibix said:
No - we'll know when the event's light cone intersects our worldline. In other words, when the light from the supernova reaches us.
Okay, okay I understand now about what light cone is, and what worldline is. Thanks for introducing me light cone and worldline. I thought they are the same. But I realize now, that they aren't. I'll contemplate your answer.

Ibix said:
But if you're happy with "the route is shorter because I took the hypotenuse", why aren't you happy with "one twin's time is longer because he took the direct route"?
"Happy" is not the word :smile:. It's just that I need a time longer to really grasp the theory.

Thanks.
 
  • #73
Ibix said:
Yes, we cannot know the supernova has started moving until it's light reaches us. That does not stop us from, after the fact, drawing a map of what must have happened. Here is a pair of space-time diagrams showing us in blue and the supernova in red. I have added dots every 500 years on each worldline.
View attachment 84886
In the left-hand diagram, the supernova is in motion and we are at rest. Note that the red dots are slightly wider spaced than the blue ones because of time dilation - there are 20 red dots and 21 blue dots. In the right-hand diagram, we are in motion and the supernova is at rest. In this frame our clocks are time-dilated, but we started them early - so there are still 20 red dots and 21 blue dots.

I haven't drawn on any light pulses because they aren't necessary to understand what's going on with the clocks. I repeat that I would advise not worrying about them - I think you are confusing yourself by trying to sort out the details of what we would see without having a grasp of the big picture.
Thanks for your trouble for answering me. It gives me enlightment. I'll contemplate your answer.
[EDIT] and graph
 
Last edited:
  • #74
Stephanus said:
"Happy" is not the word :smile:. It's just that I need a time longer to really grasp the theory.

I made graph of the two objects approaching each other on the x-axis with images of their clocks as they progress. The dots on the worldlines are clock ticks.

1. Note that all the spatial movement is in the x-direction ( or -x direction )
2. The worldlines show the progress through spacetime.
3. The time and place ( t,x) where they meet is an example of an event.
 

Attachments

  • clocks-1.png
    clocks-1.png
    3.9 KB · Views: 401
  • Like
Likes Stephanus
  • #75
Mentz114 said:
I made graph of the two objects approaching each other on the x-axis with images of their clocks as they progress. The dots on the worldlines are clock ticks.

1. Note that all the spatial movement is in the x-direction ( or -x direction )
2. The worldlines show the progress through spacetime.
3. The time and place ( t,x) where they meet is an example of an event.
Let me try to solve the problem.
clocks-1.png

At rest frame:
A speed is 11/23
C speed is 15/23
A meet C at time 23
Clock-2.JPG

Is this the space time diagram if Blue/A is rest? The Black line is the moving rest line in previous graph.
Green is green line from previous graph.
Blue is at (0,17) because ##\sqrt{23^2 - 11^2} = \sqrt{408} = 16.94##
 
  • #76
Stephanus said:
Let me try to solve the problem.
..
..
At rest frame:
A speed is 11/23
C speed is 15/23
A meet C at time 23
..
..
Is this the space time diagram if Blue/A is rest? The Black line is the moving rest line in previous graph.
Green is green line from previous graph.
Blue is at (0,17) because ##\sqrt{23^2 - 11^2} = \sqrt{408} = 16.94##

The 'shape' is right. Blue stays at x=0, green approaches and the line that was at 0,0 moves to the right.

The proper time on Blues clock is about 20.2 (counting the dots) but on your diagram the time on Blues clock is about 17. That is not right. They should be the same.

If you want to transform the diagram to Blues rest frame, you should transform the points A,B,C with a Lorentz transformation with velocity -v where v is Blues velocity.

I transformed B ( t=23, x=11) with ##\beta=-0.478, \gamma=1.138##

##x'=(11)*1.138-(0.478)*(1.138)*23=0.005##
##t'=(23)*1.138-(0.478)*(1.138)*11=20.2##

There are rounding errors but you can see that ##x'## goes to zero.

I'm encouraged that you seem to be understanding worldlines. If you complete the transformation for B and C then on the new diagram you will see

1. Invariance of proper times
2. Relativity of simultaneity.

It is worth doing.
 
Last edited:
  • Like
Likes Stephanus
  • #77
Mentz114 said:
The 'shape' is right. Blue stays at x=0, green approaches and the line that was at 0,0 moves to the right.

The proper time on Blues clock is about 20.2 (counting the dots) but on your diagram the time on Blues clock is about 17. That is not right. They should be the same.

If you want to transform the diagram to Blues rest frame, you should transform the points A,B,C with a Lorentz transformation with velocity -v where v is Blues velocity.

I transformed B ( t=23, x=11) with ##\beta=-0.478, \gamma=1.138##

##x'=(11)*1.138-(0.478)*(1.138)*23=0.005##
##t'=(23)*1.138-(0.478)*(1.138)*11=20.2##

There are rounding errors but you can see that ##x'## goes to zero.

I'm encouraged that you seem to be understanding worldlines. If you complete the transformation for B and C then on the new diagram you will see

1. Invariance of proper times
2. Relativity of simultaneity.

It is worth doing.
Hi Mentz114, thanks for your answer. I'm using someone computer now. I don't have my "spreadsheet formula" and graph with me. I'll try to make the correction later. I'm out of town now.
 
  • #78
Stephanus said:
Blue is at (0,17) because ##\sqrt{23^2 - 11^2} = \sqrt{408} = 16.94##
What? ##\sqrt{408}=16.94##? Not even 20?? I must have dozed off. Argghhh.
 
  • #79
Mentz114 said:
##x'=(11)*1.138-(0.478)*(1.138)*23=0.005##
##t'=(23)*1.138-(0.478)*(1.138)*11=20.2##

There are rounding errors but you can see that ##x'## goes to zero.
Yes, yes. You don't have to convince me. Rounding errors. But as I said, when I get back to my own computer, I'll do the calculation again. I think the green line is not right. My green line.
##\sqrt{408} = 16.94## Arghh
 
  • #80
Stephanus said:
Yes, yes. You don't have to convince me. Rounding errors. But as I said, when I get back to my own computer, I'll do the calculation again. I think the green line is not right. My green line.
##\sqrt{408} = 16.94## Arghh
'Arghh' indeed.

These diagrams are fairly accurate but not the same numbers. I won't be available for a while now.
 

Attachments

  • tt-2.png
    tt-2.png
    1.9 KB · Views: 411
  • tt-1.png
    tt-1.png
    1.7 KB · Views: 424
Last edited:

Similar threads

Back
Top