Momentum conservation in the twin paradox

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Discussion Overview

The discussion revolves around the resolution of the twin paradox within the framework of special relativity (SR), particularly focusing on the role of acceleration and momentum conservation in explaining the differential aging of the twins. Participants explore various scenarios, assumptions, and interpretations related to inertial and non-inertial frames, as well as the implications of these conditions on the paradox.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Exploratory

Main Points Raised

  • Some participants propose that the asymmetry in the twin paradox arises from the acceleration of the traveling twin, which places them in a non-inertial frame, while the stay-at-home twin remains in an inertial frame.
  • Others argue that proper times integrate to different values along different paths, and that acceleration is not necessary for the resolution of the paradox, as it is possible to construct scenarios where both twins remain in inertial frames.
  • A later reply questions the necessity of considering momentum conservation, suggesting that the stay-at-home twin can remain inertial throughout the scenario, despite the traveling twin's acceleration.
  • Some participants provide examples of scenarios where differential aging occurs without acceleration, such as one twin being launched from a cannon while the other orbits Earth.
  • Further examples include hypothetical situations involving geodesics in curved spacetime, where different paths yield different proper times, reinforcing the idea that acceleration is a convenient mechanism rather than a fundamental requirement for differential aging.
  • There is a discussion about the implications of momentum conservation and whether it necessitates that the Earth and stay-at-home twin experience any acceleration, with some participants asserting that this is not the case.

Areas of Agreement / Disagreement

Participants generally do not reach a consensus on the necessity of acceleration or inertial frames for resolving the twin paradox. Multiple competing views remain regarding the role of acceleration and the implications of momentum conservation.

Contextual Notes

Some limitations are noted, such as the dependence on specific definitions of inertial and non-inertial frames, and the unresolved nature of certain mathematical steps in the discussion. The scenarios presented vary in their assumptions and conditions, which may affect the interpretations of differential aging.

adrian_m
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I was thinking about one of the many resolutions of the so-called 'twin paradox' within SR framework. I realize many methods of resolving this have been proposed, but I am curious about the particular solution that uses 'acceleration' of the traveling twin, to create the required asymmetry for differential clock rates (time dilation) between the twins.

As I understand it, the traveling twin's clock is slowed because (s)he is in a non-inertial frame at some point(s) during the trip because of the acceleration experienced, while the stay-at-home twin always remains in an inertial frame.

However, given momentum conservation, even the Earth along with the stay-at-home twin would have to have an acceleration in the opposite direction of the traveling twin, even if by an insignificant amount. This would put the Earth and stay-at-home twin also in a non-inertial frame, however briefly.

So, what is the logic behind this particular resolution of the twin paradox that produces the asymmetry between the twins?
 
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Well the twin paradox can be done with two accelerating observers as well, in the obvious way, so the dichotomy that you mentioned is not pivotal in getting a working scenario for the paradox. The solution is simply that proper times integrate to different values along different paths.

Anyways in the scenario you're talking about we are assuming gravity has no effect/presence for the purposes of the problem hence momentum conservation associated with the gravitational interaction doesn't come into play.
 
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adrian_m said:
As I understand it, the traveling twin's clock is slowed because (s)he is in a non-inertial frame at some point(s) during the trip because of the acceleration experienced, while the stay-at-home twin always remains in an inertial frame.

Although many explanations of the twin paradox will leave you thinking this, it's not right - the acceleration does not cause the differential aging, and it's possible to set up a twin paradox in which neither twin ever experiences any acceleration and both remain in (locally) inertial frames for the duration.

The acceleration matters because, in the standard version of the paradox, it's different for the two twins. Because it's different, we can say that there is something different about the experiences of the two twins and therefore it's at least possible that the different experience includes different measurements of the passage of time. When you read a description of the standard version of the paradox, you'll always find some words along the lines of "But for the traveling twin, it's just as if he were at rest while the Earth moves away" - and because of the acceleration, it's not.

A better way of thinking about it is to say that the two twins' clocks disagree at the reunion because they took different paths of different length through space-time. The acceleration is just the mechanism which sent them on their different paths.
 
adrian_m said:
However, given momentum conservation, even the Earth along with the stay-at-home twin would have to have an acceleration in the opposite direction of the traveling twin, even if by an insignificant amount. This would put the Earth and stay-at-home twin also in a non-inertial frame, however briefly.

This is not correct. In the standard twin paradox scenario, the traveling twin fires rockets to turn around; momentum exchange with the rocket exhaust is what changes his trajectory. There is no momentum exchange with Earth or the stay-at-home twin, so the latter can be inertial the whole time.

As other posters have noted, there are other possible twin paradox-type scenarios where both twins move non-inertially; but there is no requirement that one must just because the other does.
 
adrian_m said:
However, given momentum conservation, even the Earth along with the stay-at-home twin would have to have an acceleration in the opposite direction of the traveling twin, even if by an insignificant amount.
Huh? Why is that?
 
Nugatory said:
Although many explanations of the twin paradox will leave you thinking this, it's not right - the acceleration does not cause the differential aging, and it's possible to set up a twin paradox in which neither twin ever experiences any acceleration and both remain in (locally) inertial frames for the duration.
Here is one example of differential ageing with no acceleration. One twin is fired upwards from a cannon. On leaving the atmosphere he is traveling inertially and passes his twin who happens to be orbiting the Earth. If things are set up correctly the launched twin has less than escape velocity and falls back to meet his twin who has just completed a full orbit.
I was trying to think of other examples. An elliptical orbit versus a circular orbit is problematic because of precession of the elliptical orbit. Any others?
 
yuiop said:
Any others?
Take Minkowski space-time and roll it up into a cylinder; one can find two points between which there are two time-like geodesics, one that goes straight up the cylinder and another which coils around it, and the former will record more proper time than the latter.
 
yuiop said:
Any others?
Similar to yours: One clock resting at the Earth's center. Other clock oscilating in a tunnel through the center.

Here we had some debates, if they actualy will age differently, if the oscilating clock stays within the Earth. But if it oscilates higher than the surface, then I'm pretty sure they will age differently.
 
yuiop said:
Any others?

Do the turnaround in free fall by executing a hyperbolic orbit around a massive object...
This is the case that I was thinking about when I added the "locally inertial" qualifier in my previous post.

And WbN, clever dude that he is :smile:, points out a solution that doesn't need that qualifier, although it's not one that describes our universe:
WannabeNewton said:
Take Minkowski space-time and roll it up into a cylinder; one can find two points between which there are two time-like geodesics, one that goes straight up the cylinder and another which coils around it, and the former will record more proper time than the latter.

At this point, we've moved well beyond OP's original question, although this discussion does strongly reinforce the point made above, that the acceleration is just a convenient way of introducing some asymmetry between the two travelers and sending them on different paths through spacetime, not a fundamental requirement for differential aging.
 
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  • #10
Nice answers, everyone.

WannabeNewton said:
Well the twin paradox can be done with two accelerating observers as well...
Nugatory said:
...it's possible to set up a twin paradox in which neither twin ever experiences any acceleration and both remain in (locally) inertial frames for the duration...
Instead of replying separately to everyone's answers, I am picking the above two as representative. The consensus seems to be that acceleration or inertial frames are not really necessary for the resolution.

PeterDonis said:
This is not correct. In the standard twin paradox scenario, the traveling twin fires rockets to turn around; momentum exchange with the rocket exhaust is what changes his trajectory...
True, but I think if we are going to consider non-inertial frames, the traveling twin is non-inertial three times. Is there anything specific about the 'turn around' non-inertial frame that explains his slower clock rate?

DaleSpam said:
Huh? Why is that?
I was trying to think of it in a real life scenario. Momentum conservation would have to be considered when the traveling twin departs from Earth, briefly putting even Earth in a non-inertial frame, however insignificant the acceleration (practically zero, theoretically not zero). However, as it turns out from all the answers, consideration of who is inertial throughout and who is not is unnecessary.
 
  • #11
adrian_m said:
True, but I think if we are going to consider non-inertial frames, the traveling twin is non-inertial three times. Is there anything specific about the 'turn around' non-inertial frame that explains his slower clock rate?

It's easy to get rid of the acceleration and deceleration at the two ends of the journey: Start the traveling clock in motion towards the stationary clock, set the two clocks to the same time as the traveler passes the stationary clock on the outbound leg, compare the clock readings as the traveler zooms by on his return trip. That leaves just the one acceleration at the turnaround, and we've already discussed ways of getting rid of that one as well.
 
  • #12
adrian_m said:
True, but I think if we are going to consider non-inertial frames, the traveling twin is non-inertial three times. Is there anything specific about the 'turn around' non-inertial frame that explains his slower clock rate?

Yes. Have you read the Usenet Physics FAQ on the twin paradox? And in particular, the Doppler Shift Analysis? That should make clear what the fundamental asymmetry is in the standard scenario, and why it only comes into play when the traveling twin turns around, not at the start and end of his trip, even though he is also, as you correctly note, non-inertial at the start and end of his trip.

adrian_m said:
Momentum conservation would have to be considered when the traveling twin departs from Earth, briefly putting even Earth in a non-inertial frame, however insignificant the acceleration (practically zero, theoretically not zero).

Not necessarily. The traveling twin could do his initial acceleration in a way that did not transfer any momentum to Earth (for example, by firing his rocket perfectly horizontally and achieving escape velocity in that direction).

adrian_m said:
However, as it turns out from all the answers, consideration of who is inertial throughout and who is not is unnecessary.

Correct; the Doppler Shift Analysis that I linked to above bears that out.
 
  • #13
adrian_m said:
I was trying to think of it in a real life scenario. Momentum conservation would have to be considered when the traveling twin departs from Earth, briefly putting even Earth in a non-inertial frame, however insignificant the acceleration (practically zero, theoretically not zero).
There are certainly scenarios that you could envision where there is an initial acceleration by the stay at home twin, but there are others without such acceleration. It certainly is not necessary.
 
  • #14
Thanks everyone for the resonses.
 

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