Acceleration or gravitational time dilation the same?

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Discussion Overview

The discussion revolves around the comparison of time dilation effects due to gravitational fields and acceleration, particularly in the context of General Relativity (GR) and Special Relativity (SR). Participants explore scenarios involving clocks in different gravitational potentials and those experiencing acceleration, questioning whether the time dilation effects are equivalent in these cases.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants assert that a clock near sea level on Earth runs slower than an identical clock in open space due to gravitational time dilation.
  • Others argue that in a rotating space station, the time dilation experienced by a clock under centripetal acceleration is dependent on tangential velocity rather than acceleration alone.
  • A participant suggests that the time dilation in the case of a rotating frame can be interpreted as gravitational time dilation from that perspective.
  • Some participants propose that the time dilation effects in the modified rocket scenario (one accelerating at 1g and one not) should be analyzed at the moment when both clocks have the same velocity.
  • Another viewpoint emphasizes that the time dilation factor for gravitational effects is a fixed value, while the factor for accelerating clocks can vary based on instantaneous velocity.
  • Some participants highlight that the principle of equivalence suggests that acceleration and gravity should yield the same time dilation effects, while others challenge this by stating that time dilation is related to gravitational potential rather than acceleration directly.
  • A later reply mentions that different planets with the same surface gravity can have different time dilation factors due to variations in radius and density.
  • One participant notes that there is a 1-to-1 relationship between gravitational potential and acceleration, suggesting that acceleration generates gravitational potential.

Areas of Agreement / Disagreement

Participants express differing views on whether the time dilation effects due to acceleration and gravity are equivalent. Some assert they are the same based on the principle of equivalence, while others argue that they are distinct phenomena influenced by different factors, leading to an unresolved discussion.

Contextual Notes

The discussion includes references to specific scenarios and calculations, but there are limitations in terms of assumptions about the conditions under which time dilation is analyzed, such as the effects of velocity and gravitational potential.

  • #31
Jeff Reid said:
My main question was if the equivalence principle of gravity and acceleration applies to time dilation as well.
The answer is yes. If it were otherwise then the equivalence principle wouldn't be valid.
The main difference between gravity and acceleration is that gravity changes with distance from the source, while acceleration remains constant.
It seems to me that you're speaking only of a particular gravitational field, i.e. that of a spherically symmetric body. The equivalence principle does not say that all gravitational fields are equivalent to all accelerating frames of reference. The (weak) equivalence principle states that a uniform gravitational field is equivalent to a uniformly accelerating frame of reference. The (strong) equivalence principle is about the form of equations and is known as the comma-goes-to-colon rule
So in an enclosed environment, putting two clocks at the top and bottom of a chamber, if the clocks don't run at the same speed, it's gravity (from a point source), and if they're the same, it's acceleration.
In order to observe a time dilation there must be two clocks at different gravitational potentials. Regarding an accelerating frame of reference something similar must hold. Two clocks at the same height in an accelerating frame is like being at the same gravitational potential and thus no difference in the clock rates is expected.

Pete
 
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  • #32
Jeff Reid said:
My main question was if the equivalence principle of gravity and acceleration applies to time dilation as well.

The main difference between gravity and acceleration is that gravity changes with distance from the source, while acceleration remains constant. So in an enclosed environment, putting two clocks at the top and bottom of a chamber, if the clocks don't run at the same speed, it's gravity (from a point source), and if they're the same, it's acceleration.

It can get complicated because there are various ways to artificially accelerate a rocket but generally speaking the clocks at the top and bottom of an accelerating rocket will not run at the same rate and the onboard observers will not measure them to be running at the same rate. Redshift and blueshift are observed in an artificially accelerated rocket. So the answer to the main question you ask here is yes, but your summary is not correct.
 
  • #33
My main question was if the equivalence principle of gravity and acceleration applies to time dilation as well.
Recently, I made a plot that shows gravitational time dilation in the equvalent case of two accelerated clocks. One can see immediately that the time between two light pulses is longer for the "upper" clock, according to the approximation (1+gh/c²). I don't deal with subtleties like different proper accelerations there, but this derivation of gravitational time dilation should be ok nevertheless.
 

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  • #34
Jeff Reid said:
My main question was if the equivalence principle of gravity and acceleration applies to time dilation as well.
Yes.

Please do not misunderstand my above responses. I was not stating that the equivalence principle did not hold, I was responding to the specific experimental set up you proposed in your OP which does not test the equivalence principle since it is not limited to a small (approximately flat) region of spacetime. The curvature would be detectable in the Swartzschild metric between the sea level clock and the space clock.

Jeff Reid said:
The main difference between gravity and acceleration is that gravity changes with distance from the source, while acceleration remains constant. So in an enclosed environment, putting two clocks at the top and bottom of a chamber, if the clocks don't run at the same speed, it's gravity (from a point source), and if they're the same, it's acceleration.
My understanding is that the equivalence principle holds only for small regions of spacetime where the curvature is undetectable. This type of experiment would rely on your room being big enough that you could detect the tidal gradient.
 
  • #35
Jeff Reid said:
My main question was if the equivalence principle of gravity and acceleration applies to time dilation as well.

The main difference between gravity and acceleration is that gravity changes with distance from the source, while acceleration remains constant.

That's Not true. Einstein field equation does Not imply that gravity changes with distance from the source,
It depends on the source itself. So it's possible for gravity to change very little with distance from the source or no change at all, uniform gravitational field
 
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  • #36
kahoomann said:
That's Not true. Einstein field equation does Not imply that gravity changes with distance from the source,
It depends on the source itself. So it's possible for gravity to change very little with distance from the source or no change at all, uniform gravitational field
That is quite correct. However one has to be careful in this respect because its tempting to use Newtonian intuition and as such you may arrive at the wrong answer. Consider the example of a uniform gravitational field. In Newtonian gravity the strength of the gravitational field, as measured by the gravitational acceleration ( the gravitational potential varies with height so it is not constant) is the same throughout space. In general realtivity the gravitational field is measured by the Christoffel symbols. The Christoffel symbols for a uniform gravitational field is, unlike the Newtonian case, a function of height.

Pete
 

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