A _perfectly_ symmetric twin paradox cases

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Discussion Overview

The discussion revolves around the twin paradox in the context of two proposed cases involving rockets with identical acceleration profiles. The participants explore the implications of symmetry and acceleration in special relativity (SR) and general relativity (GR), questioning how paradoxes arise in different scenarios involving observers in motion and those at rest.

Discussion Character

  • Debate/contested
  • Exploratory
  • Technical explanation

Main Points Raised

  • One participant describes two cases: one with two rockets having identical acceleration profiles traveling in opposite directions, and another with one observer on Earth and another in a rocket experiencing 1G acceleration.
  • Some participants argue that proper acceleration is independent of perspective and that gravitational time dilation disrupts symmetry in the scenarios presented.
  • Another participant emphasizes that the paths through spacetime taken by the observers are crucial, suggesting that different paths lead to different aging, regardless of acceleration profiles.
  • There is a discussion about the relevance of proper acceleration versus coordinate acceleration, with some participants clarifying that proper acceleration is what an accelerometer would measure.
  • One participant expresses confusion about the complexity of the twin paradox, likening it to the differences in distances traveled depending on the path taken in space.
  • Another participant proposes that it may be possible to arrange the rocket's thrust profile to maintain a steady 1G acceleration, questioning the implications of this for the symmetry of the cases.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the implications of symmetry in the cases discussed. There are competing views on the relevance of acceleration profiles and the nature of spacetime paths, leading to ongoing debate about the resolution of the twin paradox.

Contextual Notes

Some participants note that the discussion is complicated by the need to consider spacetime curvature and the specific paths taken by observers, which may not be fully resolved in the arguments presented.

  • #31
PeterDonis said:
In a centrifuge, the direction of "down" changes; in a rocket accelerating in a straight line, it doesn't.
Direction with respect to who ? Is a 6 degree of freedom G-meter able to distinguish (small patch locally) that we are in a centrifuge and not in a ship ?

PeterDonis said:
Also, in the OP's scenario with an observer on the surface of the Earth and an observer making a round trip from orbit to surface and back, it is impossible for the second observer's G to match the first, in either magnitude or direction, for the entire experiment.
Yes, I spot that error too, and that's why I came up with another setup which was supposed to fix this problem (by trying to make it symmetrical)
 
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  • #32
Dale said:
If your proposal was one large/fast centrifuge and one small/slow centrifuge. But you cannot apply a combination of the above 10 operations to get from one to the other, so they are not symmetric.
Thanks, that's clear now. I was applying the symmetry to each "voyager clock" separately (and locally, as the OP I think) and not appling it to transform one into the other (which seem to requires an external frame of reference, not just a local G-meter to assert symmetry)
 
  • #33
Boing3000 said:
Is a 6 degree of freedom G-meter able to distinguish (small patch locally) that we are in a centrifuge and not in a ship ?
Yes. They measure three directions of linear acceleration and three axes of rotation.
 
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  • #34
Boing3000 said:
Direction with respect to who ?

A gyroscopically stabilized local reference frame.

Boing3000 said:
Is a 6 degree of freedom G-meter able to distinguish (small patch locally) that we are in a centrifuge and not in a ship ?

Yes. See Dale's response.
 
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  • #35
Dale said:
So when we are talking about symmetry in physics this is not what we mean. In physics we talk about the symmetry of the laws of physics and the symmetry of the boundary conditions.

Well, apparently I'm not talking about "symmetry in physics" in general; in this particular context, the "symmetry" is not in the "symmetry in physics" but rather a specific reference to x2(two) records from x2(two) G-force meters observer on the Earth and observer on the rocket compare after round trip. Though, I definitely appreciate your lecturing regarding to "symmetry in physics" yet, I failed to see how it relates to the particular context, pls excuse me for my profound stupidity...
 
  • #36
stefanbanev said:
yet, I failed to see how it relates to the particular context
The particular context is a supposed difficulty with a "perfectly symmetrical" case. I was pointing out that the case is not perfectly symmetrical. So there is no difficulty. There is no expectation that the two non symmetric results should be the same.
 

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