Gravitational time dilation near Earth

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Discussion Overview

The discussion revolves around gravitational time dilation near Earth, specifically examining how the ticking rate of a clock changes with altitude and distance from the Earth, particularly in relation to the Sun's gravitational influence. Participants explore theoretical models and assumptions regarding the behavior of clocks in varying gravitational fields, including potential experimental observations.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants note that a clock on a mountain ticks faster than one at sea level, but question how this behavior changes as one moves towards the Sun.
  • There is a proposal to consider the clock on the Earth-Sun line using thrust to maintain position, with the aim of detecting a point where the clock's ticking rate begins to decrease.
  • Some participants express uncertainty about the appropriate metric to describe the gravitational effects in this scenario.
  • One participant suggests using weak field and slow motion approximations to superpose the Schwarzschild solutions for both the Earth and the Sun, leading to a specific equation for gravitational potential.
  • Another participant agrees with the superposition approach but expresses uncertainty about the limitations and assumptions involved in this method.
  • There is a discussion about the nature of time measurement, with some arguing that clocks tick at the same rate in their local frames, while others emphasize the differences in observed ticking rates due to gravitational potential differences.
  • One participant suggests that experimental techniques could be used to detect the point of inversion in ticking rates, highlighting the importance of such measurements.

Areas of Agreement / Disagreement

Participants generally do not reach a consensus on the exact nature of the gravitational effects on clock rates, with multiple competing views and uncertainties remaining about the assumptions and models proposed.

Contextual Notes

Limitations include the dependence on the assumptions of weak fields and slow motion, the potential neglect of the Earth's rotation, and the unresolved nature of the exact solution for the gravitational effects in this scenario.

  • #31
DanMP said:
In SI units, the above formula becomes

The first one you gave is correct.
 
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  • #32
Ibix said:
Optic fibres keep the FCC (or whatever your local regulatory body is) off your back and keep relatively rapidly varying atmospheric conditions from ...

What means FCC?

Do you know their method? How they compared optical clock rates?
 
  • #33
DanMP said:
What means FCC?
Federal Communications Commission. They object to unlicensed radio signals in the US - similar bodies exist elsewhere. There are plenty of ways of not annoying them - using light signals in fibres is one.
DanMP said:
Do you know their method? How they compared optical clock rates?
No. The classic experiment is the Pound-Rebka experiment, which is a really clever way of comparing the frequency of light emitted at the top of a tower to the frequency received at the bottom. The details of that aren't paywalled and are easily Googleable.
 
  • #34
PeterDonis said:
The first one you gave is correct.

Thank you!

So, we have:
$$
\phi(r_E, r_S, v_E, v_S) = 1 - \frac{GM_E}{c^2 r_E} - \frac{GM_S}{c^2 r_S} - \frac{v_E^2}{2 c^2} - \frac{v_S^2}{2 c^2}
$$

where: ##r_E=x##, ##r_S=R-x## (R=Sun-Earth distance), ##v_E=\omega x##, ##v_S=\omega (R-x)## (##\omega## = Earth's angular speed around the Sun)

So, we can write:
$$
\phi(r_E, r_S, v_E, v_S) = \phi(x)= 1 - \frac{GM_E}{x c^2} - \frac{GM_S}{(R-x) c^2} - \frac{(\omega x)^2}{2 c^2} - \frac{(\omega (R-x))^2}{2 c^2}
$$
and
$$
\frac{d \phi(x)} {dx} = \frac{GM_E}{x^2 c^2} - \frac{GM_S}{(R-x)^2 c^2} - \frac{\omega^2 x}{c^2} + \frac{\omega^2 (R-x)}{c^2}
$$

We need ##\frac{d \phi(x)} {dx} = 0##

so
$$
\frac{GM_E}{x^2 c^2} - \frac{GM_S}{(R-x)^2 c^2} - \frac{\omega^2 x}{c^2} + \frac{\omega^2 (R-x)}{c^2}=0
$$
or
$$
\frac{GM_E}{x^2} - \frac{GM_S}{(R-x)^2} - \omega^2 x+ \omega^2 (R-x)=0
$$
or
$$
\frac{GM_S}{(R-x)^2} + \omega^2 x = \frac{GM_E}{x^2} + \omega^2 (R-x)
$$

so x is the place where gravitational and centrifugal forces acting on the clock cancel each other ... Interesting.

The value is: 1,349,811,584 m
 
  • #35
DanMP said:
x is the place where gravitational and centrifugal forces acting on the clock cancel each other

Yes, that is to be expected since, in this approximation, the force is the gradient of the potential, and the potential is what determines the clock rate. So the maximum of the potential, which is where the maximum clock rate will be, is also where the gradient is zero and therefore the net force is zero.
 
  • #36
PeterDonis said:
...So the maximum of the potential, which is where the maximum clock rate will be, is also where the gradient is zero and therefore the net force is zero.

How about the opposite side of the Earth? There is a place there where the 4 forces cancel each other but, beyond it, the clock rate will continue to increase.

Is there a round the Earth transition surface? It is like the rim of the Earth's gravitational well?

What do you think about the optical clocks spiraling upwards from the Earth experiment I suggested? I have reasons to say that such an experiment is very important for relativity. I can't reveal the reasons, because personal theories are forbidden here (not the same in the other forum ... where I intend to post them in the near future), but we may find that the transition will be anything but smooth.
 
  • #37
DanMP said:
I can't reveal the reasons, because personal theories are forbidden here (not the same in the other forum ... where I intend to post them in the near future),
We thank you for respecting our rules here.

This thread is now closed. Best of luck in your academic pursuits.
 
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  • #38
DanMP said:
How about the opposite side of the Earth?

As a bit of thread cleanup, I should clarify that my statements were only referring to the potential in between the Sun and the Earth. The maximum of the potential between those bodies is only a local maximum, not a global maximum.
 
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