Find the Proper Time Extrema: Twin Paradox Explained

Ja4Coltrane
Messages
224
Reaction score
0
Quick question:
Suppose I hold two initially synchronized clocks on Earth and throw one up and catch it when it comes back down. Now my (small amount of) knowledge of GR tells me that the proper time on the thrown clock should be maximized since it was on a geodesic.

However, this seems like the twin paradox, and in the twin paradox, the thrown clock shows less time than the stationary clock.

What am I wrong about?

Thanks in advance!
 
Physics news on Phys.org
Ja4Coltrane said:
Quick question:
Suppose I hold two initially synchronized clocks on Earth and throw one up and catch it when it comes back down. Now my (small amount of) knowledge of GR tells me that the proper time on the thrown clock should be maximized since it was on a geodesic.

However, this seems like the twin paradox, and in the twin paradox, the thrown clock shows less time than the stationary clock.

What am I wrong about?

Thanks in advance!
In the twin paradox, just as in your thought experiment, the clock on geodesic (the twin who stays at home) records a longer time interval than the clock on the distorted path (the twin who flies to a far away star and comes back).
 
Ja4Coltrane said:
Suppose I hold two initially synchronized clocks on Earth and throw one up and catch it when it comes back down. Now my (small amount of) knowledge of GR tells me that the proper time on the thrown clock should be maximized since it was on a geodesic.

However, this seems like the twin paradox, and in the twin paradox, the thrown clock shows less time than the stationary clock.
You are correct. The thrown clock is on a geodesic (provided we measure from just after it leaves the thrower's hand until just before it returns) so the proper time is maximized. This is exactly analogous to the twin paradox since the thrown clock is the one that goes in a "straight" line. It travels inertially and does not measure any proper acceleration.
 
Ja4Coltrane said:
Now my (small amount of) knowledge of GR tells me that the proper time on the thrown clock should be maximized since it was on a geodesic.
I think that only holds in SR. In GR geodesic world lines maximize proper-time only locally. You can also have two geodesics meeting twice with different proper-times intervals in between.

See this thread:
https://www.physicsforums.com/showthread.php?t=249722
 
Last edited:
Either tonight or tomorrow, I'll post (some of) the fairly simple details of a GR example for which the usual SR result doesn't hold, i.e., the elapsed proper time between meetings for an accelerated clock is greater than for a non-accelerated (geodesic) clock.

The example consists of two clocks that have same r, with one clock in geodesic circular orbit (freely falling with no acceleration) and one clock hovering (accelerated).
 
Ja4Coltrane said:
However, this seems like the twin paradox, and in the twin paradox, the thrown clock shows less time than the stationary clock.

You're misidentifying which clock in the Twin Paradox is the "thrown" clock. In that example, it is the twin that remains on Earth that is analogous to the clock you throw in your own example. In the twin paradox, we are ignoring effects of gravity (which are minimal in any case), so we're really talking about a freely-floating twin (in place of the Earth) and a twin that goes to Vega and accelerates when he gets there. The accelerated twin knows that it was he who accelerated because he feels the acceleration (the acceleration is recorded by an accelerometer, i.e. it causes a mass-on-a-spring to stretch).

In your example, it is the earthbound clock whose accelerometer stretches, while the freely falling clock experiences zero acceleration. Hence the freely falling clock will have the extreme aging.

Note, however, that while in SR you are guaranteed that the inertial observer will have aged by the maximum amount, in GR you are only guaranteed that inertial observers (with no acceleration on their accelerometers) age by extreme amounts. That amount could be maximum, minimum, or even a saddle point. In this example, however, it will indeed be maximum.
 
OK, so this has bugged me for a while about the equivalence principle and the black hole information paradox. If black holes "evaporate" via Hawking radiation, then they cannot exist forever. So, from my external perspective, watching the person fall in, they slow down, freeze, and redshift to "nothing," but never cross the event horizon. Does the equivalence principle say my perspective is valid? If it does, is it possible that that person really never crossed the event horizon? The...
In this video I can see a person walking around lines of curvature on a sphere with an arrow strapped to his waist. His task is to keep the arrow pointed in the same direction How does he do this ? Does he use a reference point like the stars? (that only move very slowly) If that is how he keeps the arrow pointing in the same direction, is that equivalent to saying that he orients the arrow wrt the 3d space that the sphere is embedded in? So ,although one refers to intrinsic curvature...
ASSUMPTIONS 1. Two identical clocks A and B in the same inertial frame are stationary relative to each other a fixed distance L apart. Time passes at the same rate for both. 2. Both clocks are able to send/receive light signals and to write/read the send/receive times into signals. 3. The speed of light is anisotropic. METHOD 1. At time t[A1] and time t[B1], clock A sends a light signal to clock B. The clock B time is unknown to A. 2. Clock B receives the signal from A at time t[B2] and...
Back
Top