If No, well this can't be, as there is perfect symmetry, you can't tell one from the other.

If Yes, they had relative velocities all along, then their times must have dilated and somehow they must not agree with each other.

P.S I know I am wrong, please help me find out where.

P.P.S For all those who are marking this as a duplicate question of What is the proper way to explain the twin paradox?, I think this is not same as plain old twin paradox because its made symmetric and the essence of the question is not how do you solve twin paradox, instead it is why is this not like twin paradox?

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    $\begingroup$ According to their Mom, who stayed home, both twins left at noon, turned around at 1:00, and got back home at 2:00. Twin A says: "My clock ran really slow till I turned around, but now it's running normally. Your clock ran normally till you turned around, but now it's running really slow. Now mine has just caught up with yours, so they agree. They both say 1:30." Twin B says exactly the same thing. Perfectly symmetric. $\endgroup$
    – WillO
    Apr 28 '18 at 16:44
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    $\begingroup$ Possible duplicate of What is the proper way to explain the twin paradox? $\endgroup$ Apr 28 '18 at 21:34

Yes, the two twins (with the same there-and-back speeds) would, upon their reunion, have aged the same.

Here's a spacetime diagram on "rotated graph paper" that displays the symmetry of the travelers. (The rotated graph paper helps us draw the clock ticks along various observer worldlines.) You could use this diagram to support various ways (e.g. from the other given answers) to explain the result that these twins would age the same.

The travelers each have there-and-back speeds of $(3/5)c$.

I have displayed each observer's lines of simultaneity, just before and just after her turn-around events. These are associated with relative-simultaneity and time-dilation.

I have also displayed the periodic transmissions by the initially-forward twin, and the receptions by the initially-backward twin. This shows what the initially-backward twin would "see". These are associated with the Doppler effect. (You can draw the corresponding transmissions by the initially-backward twin.)

Clock Effect Two Travelers - Relativity on Rotated Graph Paper

  • 1
    $\begingroup$ Thanks for the answer, this means a lot to me, just one more clarification, the above space time diagram is from the reference of M, but if we use the reference of P'', we will get the space time diagram of the classical twin paradox which predicts time disagreement between the twins. So what my question is this how is this different from the classical twin paradox? (I know acceleration is not the key, thanks to youtube.com/watch?v=GgvajuvSpF4 ), and if not for acceleration the classical twin paradox and this are essentially the same thing $\endgroup$ Apr 28 '18 at 18:04
  • $\begingroup$ You can redraw the spacetime diagram from the viewpoint of the inertial observer OP''... but not from the non-inertial [although piecewise-inertial] observer OP''Z. If you tried to draw such a diagram, you'll find that it is not equivalent to an inertial-observer's diagram (since it's not obtainable by a Lorentz Transformation). So, it won't be the twin-paradox diagram like the one drawn by observer OMZ. In fact, OP''Z's diagram may miss some events in spacetime or have two distinct points referring to the same event... depending on how you assign coordinates to distant events (not on OP''Z). $\endgroup$
    – robphy
    Apr 28 '18 at 18:18
  • $\begingroup$ In fact, you can compare how inertial observer OMZ and non-inertial observer OP''Z "sees" OP'Z's transmissions. Inertial observer OMZ sees two phases, while non-inertial observer OP''Z sees three phases. $\endgroup$
    – robphy
    Apr 28 '18 at 18:25
  • $\begingroup$ I'm sorry, out three phases seen by OP"Z the middle phase is neutral, i.e the twins are in rest with each other, this is as good as the classical twin staying some time unmoving in alpha centuri and returning back, even then we would still expect him to be younger, right? $\endgroup$ Apr 28 '18 at 18:36
  • $\begingroup$ The part about the phases is to suggest that the non-inertial observer OP''Z will not view OPZ's transmissions like inertial observer OMZ does. In other words, OP''Z can never be viewed as inertial. $\endgroup$
    – robphy
    Apr 28 '18 at 18:42

Yes. Once the twins reunited, they would discover that they had aged the same amount of time.

This assumes that the twins return to their initial location, and that their paths have the same shape with respect to that location, but in different directions.

This must be true, because an observer who remained behind at the fixed location must see the same amount of time pass for either twin, regardless of the direction that the particular twin initially left that location.

During the journey, each twin would see the other twin's clock change at varying rates, depending on their relative velocity. However, once the twins returned to their initial location, the clocks would show identical values.

The following illustration shows what happens from the point of view of the stationary observer who remains home, and the values that appear on the clocks when the twins leave and when they return. The exact numbers would depend on the speed of the twins relative to the stationary observer and the distance traveled.

enter image description here

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    $\begingroup$ Thanks, just one more clarification, the above space time diagram is from the reference of Earth, but if we use the reference of a twin, we will get the space time diagram of the classical twin paradox which predicts time disagreement between the twins. So my question is this how is this different from the classical twin paradox? (I know acceleration is not the key, thanks to youtube.com/watch?v=GgvajuvSpF4 ), and if not for acceleration the classical twin paradox and this are essentially the same thing $\endgroup$ Apr 28 '18 at 18:10
  • $\begingroup$ The difference between the problem you posed and the classical twin paradox is that the paths of the moving twins (the blue and red lines) are symmetrical. In the classical twin paradox (the green and red lines), the paths are not symmetrical. $\endgroup$
    – Drew
    Apr 28 '18 at 18:36
  • $\begingroup$ Upvoting this answer since it is the only one that mentions "proper time". This is the key to understanding all versions of the twin paradox. Proper time is defined as the elapsed local time for an observer on a particular path, and it is an invariant, i.e. it is independent of what coordinates you use when you calculate it. And just like the shortest path in 3D-space is a straight line, the longest path in 4D minkowski spacetime is an inertial-motion timeline. $\endgroup$
    – Cuspy Code
    Apr 28 '18 at 20:06
  • $\begingroup$ @CuspyCode I believe that the colored rectangles in the diagram that robphy posted represent units of proper time, although this was not called out explicitly. $\endgroup$
    – Drew
    Apr 28 '18 at 20:28

Here's another way of thinking about it that might be helpful.

For the classical twin paradox, twin A is at rest and twin B travels away and comes back.

Imagine that each twin measures time using a "light clock", which is a pair of mirrors with a photon bouncing back and forth between them. Each time a mirror is stuck by a photon, this is interpreted as a tick of the clock.

In the following diagram, space is on the horizontal axis, and time is on the vertical axis.

enter image description here

The blue lines are the paths of photons bouncing between the mirrors, which are the vertical or angled gray lines. Because the mirrors for twin B are moving at a significant fraction of the speed of light, it takes longer for the photon moving in the direction of the mirrors to catch up with them, and consequently the ticks are farther apart.

Twin A would observe that twin B's ticks are spaced farther apart, and therefore that twin B's time seems to be passing more slowly. However, twin B, traveling along with his clock, would always see the ticks happening at what he perceived as normal speed, since the clock would, by definition, measure the rate at which time was passing for him.

When twins A and B meet when twin B returns from his journey, twin A has counted 11 ticks, and twin B has counted 6 ticks.

For the extended twin paradox problem that you proposed, a third twin, C, would travel to the left of twin A and back, with a path otherwise identical to twin B. Twin C would also therefore count 6 ticks.

What if there was no stationary twin A, and just the two moving twins, B and C? They would still count 6 ticks each.

Using this kind of presentation, just concentrate on the paths of the photons between the mirrors and how many ticks of time are experienced by each of the twins.

What do you think of that way of thinking about it?

  • $\begingroup$ That's essentially what I did on my diagram on rotated graph paper. In earlier presentations of my diagram, I included the worldlines of the light-clock mirrors. But they are implied by set of spacelike-related corners in a sequence of light-clock diamonds. $\endgroup$
    – robphy
    Apr 28 '18 at 20:07
  • $\begingroup$ (By the way, the separation of the mirrors for B have to smaller than the mirrors for A (in A's diagram) due to length contraction.) $\endgroup$
    – robphy
    Apr 28 '18 at 20:15
  • $\begingroup$ @robphy Thanks for the clarification. I did suspect that the diagrams were related. Also, I agree that B's mirrors should be closer together. This is an old diagram I made a while ago for myself, and I only realized recently that the mirror distance is wrong. In the context of Chakrapani's question, however, I felt that the diagram was nevertheless sufficient to explain the scenario in general times. $\endgroup$
    – Drew
    Apr 28 '18 at 20:23

Yes, they would. Symmetry applies.

Suppose they start together at $t=0$ going with relative speed $v={3 \over 5} c$, (so $\gamma=1.25$) in opposite directions for a pre-agreed 5 days (each by their own clock). Each would say that when they did so, their twin's clock was running slow by a factor of 4/5.

Then they both slow down and reverse their direction of travel: we can assume this takes no significant time. When the stress of turnaround is over, they will each say that although their own clock is still showing 5, their twin's clock has jumped from 4 to 6.

The return journey takes 5 days, during which their twins clock runs slow again adding only 4 days, so both show 10 days at the end.

As always "A says B's clock shows $t_1$ when their own says $t_2$" means "A receives a picture of B's clock, showing $t_1$, at some time $t_3$: they correct for the transit time $\Delta$ and report $t_2=t_3-\Delta$. If the separation distance when the signal arrives is $X$ then $c\Delta=X+v\Delta$. On changeover the sign of $v$ changes, causing the jump in their evaluation of their twin's clock measurements.

The nice thing about relativity paradoxes is that they always have an answer.

  1. yes they would have aged the same

  2. you are saying if yes, then their times must have dilated and they must not agree

  3. but what you are missing is that it is not speed that counts, because speed is symmetrically relative, but what matters is acceleration, because that is absolute

  4. if they travel with constant speeds, then they only age less compared to the third twin (lets say there is a third twin on Earth) on Earth when they must decelerate at the point of return

  5. that is the moment when because of deceleration (which is the same effect as gravity) the twins on the spaceships slow down in the time dimension

  6. their four speed vector's magnitude must stay c, and if their spatial speed decelerates, their speed in the time dimension must slow down to compensate for the change in their spatial speed

  7. so at the point of turn, they slow down in the time dimension compared to the third twin, and they age less, and the third twin ages more

  8. but the two twins on the spaceships undergo acceleration/deceleration the same way symmetrically so their speed in the time dimension is the same, so they do not age compared to each other


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