Do clocks remain synchronized forever according to the equivalence principle?

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Discussion Overview

The discussion revolves around the synchronization of clocks in the context of the equivalence principle, particularly comparing a clock held by Jim on Earth and another clock held by Bill in a rocket ship accelerating at 1g. Participants explore whether these clocks remain synchronized indefinitely under the assumption of a homogeneous gravitational field.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Exploratory

Main Points Raised

  • Bob questions if Jim's and Bill's clocks should remain synchronized forever due to the equivalence principle, suggesting that the website's claims about relative aging may be misleading.
  • Some participants clarify that the equivalence principle applies to local observations in small regions of spacetime and does not guarantee that clocks will remain synchronized over larger distances or timeframes.
  • One participant notes that if the relative velocity between Jim and Bill is zero, their clocks could remain synchronized, but if they are in motion relative to each other, special relativity time dilation must be considered.
  • There is a discussion about whether, upon Bill's return to Earth, the two clocks would read the same, with some asserting that they would not necessarily do so due to the effects of spacetime curvature over significant distances.

Areas of Agreement / Disagreement

Participants express differing views on whether the clocks will remain synchronized, with some asserting that synchronization is contingent on relative motion and others emphasizing the limitations of the equivalence principle in this context. The discussion remains unresolved regarding the implications of these factors on clock synchronization.

Contextual Notes

Limitations include the dependence on the definitions of synchronization and the equivalence principle, as well as the unresolved nature of how significant distances and time affect clock readings.

Bob Walance
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I did do some searching on this site for an answer to this, but couldn't find exactly what I was looking for. So, here it goes:

First -- assume that the gravitational field that Jim experiences is "homogenous" (that is, constant magnitude and direction within his region of spacetime).


Jim is standing on the Earth and is holding a clock. Bill, who has a similar clock, is in a rocket ship that is accelerating at a constant 1g (as measured by the body weight scale that Bill is standing on).

1 - Since, according to Einstein, these two cases are "equivalent", then shouldn't Jim's and Bill's clocks remain synchronized forever?

If this is true, then what this website says about relative aging is misleading.

http://math.ucr.edu/home/baez/physics/Relativity/SR/rocket.html

It seems, rather, that a clock in an inertial frame of reference, for example a clock on a satellite, would age differently than Jim's and Bill's clocks.

2 - In this case the satellite is in 0g and Bill and Jim are at 1g, then after 5 years have elapsed on Bill's and Jim's clocks the satellite's clock will have aged 83.7 years, correct?

Thanks for any insight into this.

Bob Walance
 
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Bob Walance said:
1 - Since, according to Einstein, these two cases are "equivalent", then shouldn't Jim's and Bill's clocks remain synchronized forever?
The equivalence principle just says that if they each make local observations--observations in a very small patch of space around them, over a brief amount of time (technically the equivalence is only exact if the space and time are infinitesimally small)--then they will see the same results if they perform identical experiments. The equivalence principle does not imply that if they are observing each other over a large distance and a significant period of time, that they will each observe the other's clock to be ticking at the same rate...the rate each sees would depend on the geometry of the whole spacetime and their relative positions in it.
 
JesseM said:
The equivalence principle just says that if they each make local observations--observations in a very small patch of space around them, over a brief amount of time (technically the equivalence is only exact if the space and time are infinitesimally small)--then they will see the same results if they perform identical experiments. The equivalence principle does not imply that if they are observing each other over a large distance and a significant period of time, that they will each observe the other's clock to be ticking at the same rate...the rate each sees would depend on the geometry of the whole spacetime and their relative positions in it.

So, if the space traveler returns to Earth, and assuming he orients his spacecraft to maintain his 1g acceleration the entire time, will the two clocks read the same?

Thanks,
Bob
 
Bob Walance said:
I did do some searching on this site for an answer to this, but couldn't find exactly what I was looking for. So, here it goes:

First -- assume that the gravitational field that Jim experiences is "homogenous" (that is, constant magnitude and direction within his region of spacetime).


Jim is standing on the Earth and is holding a clock. Bill, who has a similar clock, is in a rocket ship that is accelerating at a constant 1g (as measured by the body weight scale that Bill is standing on).

1 - Since, according to Einstein, these two cases are "equivalent", then shouldn't Jim's and Bill's clocks remain synchronized forever?
Yes, if the relative velocity between them is zero. If not, then you have to account for SR time dilation.

And the equivalence principle says that Jim and Bill will get the same results for any local experiment they each perform. It doesn't say that each one's clock will read the same as the other. That would only be true if they were stationary with respect to each other, like if the rocket were 10 ft off the ground accelerating to oppose gravity, and Jim is 10 ft off the ground on a ledge next to the ship. Then their clocks would stay in synch with each other.
 
Bob Walance said:
So, if the space traveler returns to Earth, and assuming he orients his spacecraft to maintain his 1g acceleration the entire time, will the two clocks read the same?
No, not necessarily. Again, the equivalence principle is only about experiments which take place entirely in one small piece of spacetime--an experiment that involves starting out with synchronized clocks, then moving apart some significant distance for a significant time, then coming together and comparing clocks again, is not an experiment confined to a tiny region of spacetime where the effects of spacetime curvature can be considered negligible.
 

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