Time Dilation: Accelerating vs Inertial Frame

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Discussion Overview

The discussion centers around the concept of time dilation in the context of special relativity, specifically comparing the effects of acceleration versus constant velocity. Participants explore the implications of a scenario where a ship accelerates at 1g for one hour versus another ship moving at a constant speed of 1610 km/s, both as observed from a stationary frame. The conversation includes theoretical considerations, mathematical reasoning, and interpretations of specific examples from a referenced paper.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • Some participants express surprise that both an accelerating ship and an inertial ship can show the same amount of time dilation, questioning the role of acceleration in this context.
  • One participant argues that time dilation is based solely on instantaneous velocity relative to a rest frame, suggesting that the path taken to reach that velocity does not matter.
  • Another participant challenges the correctness of the referenced paper's equations, asserting that there is no general equivalence between gravity and acceleration, and that the time dilation experienced by an accelerating clock differs from that of a clock moving at constant velocity.
  • Some participants agree that the Lorentz gamma factor applies equally regardless of how speed is attained, but note that the elapsed time for an accelerating object differs from that of an inertial object due to varying gamma factors during acceleration.
  • Mathematical expressions are provided to illustrate the differences in proper time experienced by an accelerating rocket versus an inertial one, emphasizing the nuances in their respective time dilation effects.
  • A participant expresses gratitude for clarifications, reinforcing the idea that only instantaneous velocity affects time dilation, while questioning the reliability of the referenced paper's conclusions.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the implications of acceleration for time dilation. While some agree on the role of instantaneous velocity, others challenge the interpretations and calculations presented in the referenced paper, indicating ongoing disagreement and uncertainty.

Contextual Notes

Participants note limitations in the referenced paper's equations and reasoning, particularly regarding the treatment of acceleration and its effects on time dilation. There are unresolved mathematical steps and differing interpretations of the relationship between acceleration and time dilation.

Buckethead
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This is probably common knowledge to relativity aficionados but at Example 7.3 in this paper:

https://www.farmingdale.edu/faculty/peter-nolan/pdf/relativity/Ch07Rel.pdf

I was surprised to read the author showing that a ship accelerating at 1g from rest for 1 hour and reaching a speed of 1610km/s as seen by a stationary observer will show exactly the same amount of dilation as another ship flying past the same observer for 1 hour at a speed of 1610km/s. The amount of dilation in both cases is 1.0000144 hr.

The reason I find this counter-intuitive is obvious. The accelerating ship is not going at the maximum speed during the whole trip as is the inertial ship, so I would have thought it would show less dilation.

I thought about this and realized the difference must lie in the fact that the accelerating ship is experiencing gravity in addition to velocity which the inertial ship is not. And since gravity slows time, it is this gravity due to acceleration that is making the two equal.

Is my realization correct? I have read in other threads in this forum that acceleration (i.e. a ship accelerating) does not affect time dilation, only the resulting velocities at each point matter. I apologize that I cannot refer to such posts, but I remember them being in response to questions about the twin paradox. But if that were true, then the two times should be different due to the differences in the sums of the instantaneous velocities during acceleration. Can someone clarify this? Thanks.
 
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Time dilation is an observation from a "rest frame" of an object in that rest frame that has non-zero velocity. It doesn't have an "amount", just an instantaneous value based on the velocity relative to the rest fame, so if objects at time T are going the same speed in the rest frame, it's irrelevant how they got to that speed, they will have the same value of time dilation.

Now, differential aging is different and can depend on total path-velocity.
 
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Buckethead said:
This is probably common knowledge to relativity aficionados but at Example 7.3 in this paper:

https://www.farmingdale.edu/faculty/peter-nolan/pdf/relativity/Ch07Rel.pdf

I was surprised to read the author showing that a ship accelerating at 1g from rest for 1 hour and reaching a speed of 1610km/s as seen by a stationary observer will show exactly the same amount of dilation as another ship flying past the same observer for 1 hour at a speed of 1610km/s. The amount of dilation in both cases is 1.0000144 hr.

The reason I find this counter-intuitive is obvious. The accelerating ship is not going at the maximum speed during the whole trip as is the inertial ship, so I would have thought it would show less dilation.

I thought about this and realized the difference must lie in the fact that the accelerating ship is experiencing gravity in addition to velocity which the inertial ship is not. And since gravity slows time, it is this gravity due to acceleration that is making the two equal.

Is my realization correct? I have read in other threads in this forum that acceleration (i.e. a ship accelerating) does not affect time dilation, only the resulting velocities at each point matter. I apologize that I cannot refer to such posts, but I remember them being in response to questions about the twin paradox. But if that were true, then the two times should be different due to the differences in the sums of the instantaneous velocities during acceleration. Can someone clarify this? Thanks.

I agree with you. The time dilation in the scenario he describes is entirely due to the relative velocity at each point in time. In particular, a clock that accelerates from rest to some speed ##v## cannot record the same proper time as a clock that travels at speed ##v## throughout, as measured in some IRF.

Also, his equation (7.38) is wrong. There is no general equivalence between "gravity" and "acceleration". The equivalence is between "gravity" and an "accelerating reference frame".

In equation (7.32) the distance ##y## refers to the distance between two clocks that are both in an accelerating reference frame. This cannot be replaced with the total distance traveled by a single acclerating clock as measured in an inertial reference frame.

That section, IMHO, is all nonsense.

PS equation 7.38 gives the rate of time dilation once a distance ##y## has been travelled. But, of course, the proper time of the clock is the integral of this factor. Not simply this final time dilation factor multiplied by the coordinate time of the motion!

In any case, the logic of this whole section is totally wrong.
 
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Buckethead said:
The amount of dilation in both cases is 1.0000144 hr.
Agree with @PeroK. It is true that the Lorentz gamma factor of something doing ##v## is the same however the object attained that speed. But that means that, working in an inertial frame, the elapsed time for an object during coordinate time ##T## is $$\int_0^T\frac{dt}{\gamma(t)}$$which is obviously not the same for an object where ##\gamma(t)## is a constant and where ##\gamma(t)=\sqrt{1-(at/c)^2}##.
 
If a rocket with constant proper acceleration (magnitude ##\alpha##) starts from rest, then after a duration ##c \Delta t## of a qualifying inertial observer's coordinate time (qualifying here means that the rocket's motion is rectilinear), the final rapidity of the rocket in that frame is:

##\phi = \sinh^{-1}\left( ( \alpha / c^2) c \Delta t \right)##,

and the elapsed proper time for the rocket is:

##c \Delta \tau_{accelerating} = \dfrac{\phi}{ \alpha / c^2} ##

(see here).

If a second inertial rocket were moving with the first rocket's final rapidity ##\phi## for that same duration of observer coordinate time ##c \Delta t##, its elapsed proper time would be less:

##c \Delta \tau_{inertial} = \dfrac{c \Delta t}{\cosh \phi}##

(that's just the time dilation formula).

With ##\Delta t = 1## hour and ##\alpha = 1## g:

##\Delta \tau_{accelerating} \approx 3599.99999## seconds
##\Delta \tau_{inertial} \approx 3599.99998## seconds.

[Edited to correct 3999 to 3599]
 
Thank you all very much for your answers. I'm glad I can take to the bank the fact that only instantaneous velocity and not acceleration have an effect on time dilation. What a surprise to see such a well written paper as being so wrong. It's hard to sort out what's true from what's not when something is presented so well such as in this paper.
 
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