Resolving the Twin Paradox: Non-Straight Paths and Proper Time in Space-Time

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SUMMARY

The twin paradox is resolved by understanding that in Minkowski spacetime, the proper time is maximized along straight paths between two events. Any non-straight path results in less proper time, contradicting the assumption that a longer trajectory equates to more elapsed time. The proper time can only be accurately measured along a specified path, and the spacetime interval is defined by the equation ds^2=-c^2 dt^2 + dx^2 + dy^2 + dz^2. Thus, the twin who travels along a straight path will age more than the one who takes a curved trajectory.

PREREQUISITES
  • Understanding of Minkowski spacetime geometry
  • Familiarity with the concept of proper time in relativity
  • Knowledge of spacetime intervals and their mathematical representation
  • Basic principles of special relativity
NEXT STEPS
  • Study the mathematical formulation of Minkowski spacetime
  • Explore the implications of proper time in different trajectories
  • Learn about spacetime intervals and their applications in physics
  • Investigate the differences between Euclidean and Minkowski geometries
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Physicists, students of relativity, and anyone interested in the nuances of spacetime and the twin paradox will benefit from this discussion.

Ahmed1029
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Is the twin paradox settled by saying that any non-straight path between two events (points) in space-time has less proper time that a straight path between the two events? So the twin in the frame which has a longer trajectory between the two pints(curved) will have less elapsed time?
 
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Ahmed1029 said:
Is the twin paradox settled by saying that any non-straight path between two events (points) in space-time has less proper time that a straight path between the two events?
Yes.

Ahmed1029 said:
So the twin in the frame which has a longer trajectory between the two pints(curved) will have less elapsed time?
No. Be careful not to mix in your Euclidean thinking into the argumentation. ”Longer” in spacetime equates to larger proper time and so the ”longer” path is the straight path. The only geometry you should be referring to is the Minkowski geometry of spacetime.
 
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Orodruin said:
No. Be careful not to mix in your Euclidean thinking into the argumentation. ”Longer” in spacetime equates to larger proper time and so the ”longer” path is the straight path. The only geometry you should be referring to is the Minkowski geometry of spacetime.
I implicitly assume flat spacetime, so it's right in this context right?
 
Ahmed1029 said:
I implicitly assume flat spacetime, so it's right in this context right?
No. You are implicitly assuming Euclidean spacetime rather than Minkowski spacetime. Both are flat but only the latter is the spacetime relevant to special relativity.
 
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Orodruin said:
No. You are implicitly assuming Euclidean spacetime rather than Minkowski spacetime. Both are flat but only the latter is the spacetime relevant to special relativity.
but in Minkowski spacetime, the interval is equal to the proper time only when the observer moving in a straight line between the events. If it deviates from the straight line, it's not enough to measure the coordinate time for that frame to say it's equal to the distance of its spacetime trajectory and thus shorter than the straight trajectory
 
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Orodruin said:
No. You are implicitly assuming Euclidean spacetime rather than Minkowski spacetime. Both are flat but only the latter is the spacetime relevant to special relativity.
Ah but I could measure its proper time between infinitesimally close points along its own trajectory and they're going to add up to less than that of a straight line. Got the point thanks
 
Ahmed1029 said:
the interval is equal to the proper time only when the observer moving in a straight line between the events
This can be some (IMO) bad terminology by certain authors who define the spacetime interval or the proper time between events. They should both be defined along a path rather than between events.

The interval should be ##ds^2=-c^2 dt^2 + dx^2 + dy^2 + dz^2## and the proper time should be ##d\tau^2=-ds^2/c^2##. Both of these are then integrated along a specified path to get the interval, ##s##, or proper time, ##\tau##.
 
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Dale said:
This can be some (IMO) bad terminology by certain authors who define the spacetime interval or the proper time between events. They should both be defined along a path rather than between events.

The interval should be ##ds^2=-c^2 dt^2 + dx^2 + dy^2 + dz^2## and the proper time should be ##d\tau^2=-ds^2/c^2##. Both of these are then integrated along a specified path to get the interval, ##s##, or proper time, ##\tau##.
Yeah, I was confused at first because I thought proper time had to be only defined for straight paths. Nevertheless, the strights path traveller ages absolutely more than the one who moves on a curved path, am I correct?
 
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Ahmed1029 said:
the strights path traveller ages absolutely more than the one who moves on a curved path, am I correct?
Yes. With @Orodruin ’s caution that we are talking about paths in spacetime, not paths in space.
 
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