Acceleration of a Satellite in General Relativity

In summary, the expression for motion of a satellite in a geocentric reference frame is given by: - Delta \ddot{\mathbf{r}} = \frac{GM_E}{c^2r^3} \left\{\left[2(\beta+\gamma)\frac{GM_E}{r} - \gamma \dot{\mathbf{r}} \cdot \dot{\mathbf{r}} \right] \mathbf{r} + 2(1+\gamma)(\mathbf{r}\cdot\dot{\mathbf{r}})\dot{\mathbf{r}} \right\} + (1+\gamma)\frac
  • #1
Matter_Matters
36
2
Hi there guys,

I'm struggling! I've been looking at the International Earth Rotation Services (IERS) "standards" for motion of a satellite in GR. the expression is far from trivial and I'm battling to determine where to even start with this bad boy.

The expression is given by

[tex]
\Delta \ddot{\mathbf{r}} = \frac{GM_E}{c^2r^3} \left\{\left[2(\beta+\gamma)\frac{GM_E}{r} - \gamma \dot{\mathbf{r}} \cdot \dot{\mathbf{r}} \right] \mathbf{r} + 2(1+\gamma)(\mathbf{r}\cdot\dot{\mathbf{r}})\dot{\mathbf{r}} \right\} + (1+\gamma)\frac{GM_E}{c^2r^3} \left[ \frac{3}{r^2}(\mathbf{r}\times\dot{\mathbf{r}})(\mathbf{r}\cdot\mathbf{J})+(\dot{\mathbf{r}}\times \mathbf{J})\right] + \left\{ (1+2\gamma)\left[\dot{\mathbf{R}} \times \left( \frac{-GM_S \mathbf{R}}{c^2R^3} \right) \right] \times\dot{\mathbf{r}} \right\}.
[/tex]

The terms in the expression correspond to the following:
[itex]c = [/itex] speed of light.
[itex] \beta, \gamma [/itex] = PPN (parameterized post-Newtonian) parameters, equal to 1 in General Relativity.
[itex] \mathbf{r} [/itex] is the position of the satellite with respect to the Earth.
[itex] \mathbf{R} [/itex] is the position of the Earth with respect to the Sun.
[itex] J [/itex] is the Earth’s angular momentum per unit mass.
[itex] GM_E [/itex] and [itex] GM_S [/itex] are the gravitational coefficients of the Earth and Sun, respectively.

Now, obviously nobody in their right mind is going to know how to derive this monster off the top of their heads, unless of course you wrote the technical note, BUT, does anyone have experience with Relativistic mechanics of satellite is geocentric reference frame or barycentric for that matter?
 
Last edited:
Physics news on Phys.org
  • #2
I don't know if this will help, but the approach that comes to mind is to first find what metric the IERS is using for the Earth-sun-satellite system. The next step is to say that the satellite is following a geodesic of said metric, and write the geodesic equations.

To "simplify" things, it looks like they're using 3-vector notation rather than tensors, as evidenced by the use of cross products, which are only defined in 3 dimensions. These are presumably there to account for the effects of the Earths orbital and rotational angular momentum on the metric.

Presumably they're using some variant of the PPN metric, it rather looks like the same version MTW uses in Gravitation, due to the presence of beta's and gamma's. There are a couple of different versions of the PPN metric out there (at least according to Wikipedia.) It doesn't look (to me) like they're using the same symbolism as the IAU recommends for their solar system metric in the IAU 2000 resolutions, https://syrte.obspm.fr/IAU_resolutions/Resol-UAI.htm, or the 2006 ammendments of the resolutions (which I don't have a link to).

I got a link error when I tried to look at the technical note, I'll try again.
 
  • Like
Likes Matter_Matters
  • #3
pervect said:
I don't know if this will help, but the approach that comes to mind is to first find what metric the IERS is using for the Earth-sun-satellite system. The next step is to say that the satellite is following a geodesic of said metric, and write the geodesic equations.

So my very limited knowledge is that they are following the Schwarzschild metric including both Lens-Thirring and DeSitter effects. It is quite confusing because the documentation is a derivative with respect to coordinate time also and not proper time, like one would expect in relativity.

pervect said:
To "simplify" things, it looks like they're using 3-vector notation rather than tensors, as evidenced by the use of cross products, which are only defined in 3 dimensions. These are presumably there to account for the effects of the Earths orbital and rotational angular momentum on the metric.

I think you are right as these terms correspond to frame dragging and precession.

pervect said:
Presumably they're using some variant of the PPN metric, it rather looks like the same version MTW uses in Gravitation, due to the presence of beta's and gamma's. There are a couple of different versions of the PPN metric out there (at least according to Wikipedia.) It doesn't look (to me) like they're using the same symbolism as the IAU recommends for their solar system metric in the IAU 2000 resolutions, https://syrte.obspm.fr/IAU_resolutions/Resol-UAI.htm, or the 2006 ammendments of the resolutions (which I don't have a link to).

I got a link error when I tried to look at the technical note, I'll try again.

My intuition is saying that it is some PPN approximation of the Schwarzschild metric. I've updated the link, hopefully it works now. Thanks for the reply.
 
  • #4
There's more than just the Schwarzschild metric in there, as they have effects from the Earth and the Sun included. The Schwarzschild metric would include effects from only one dominant mass.

The PPN formalsim can handle that (approximately) though.
 
  • Like
Likes Matter_Matters
  • #5
pervect said:
There's more than just the Schwarzschild metric in there, as they have effects from the Earth and the Sun included. The Schwarzschild metric would include effects from only one dominant mass.

The PPN formalsim can handle that (approximately) though.
I think it's time to start reading up and giving some proper attention to the PPN formalism! Cheers.
 

Related to Acceleration of a Satellite in General Relativity

1. What is the difference between acceleration in Newtonian mechanics and general relativity?

In Newtonian mechanics, acceleration is defined as the rate of change of velocity with respect to time. However, in general relativity, acceleration is defined as the rate of change of spacetime curvature with respect to time. This means that in general relativity, acceleration is not just caused by a force acting on an object, but also by the curvature of spacetime caused by massive objects.

2. How does general relativity explain the acceleration of a satellite in orbit?

According to general relativity, the acceleration of a satellite in orbit around a massive object, such as the Earth, is caused by the curvature of spacetime. The satellite is constantly falling towards the Earth due to the gravitational pull, but because of its high velocity, it is able to maintain a stable orbit instead of crashing into the Earth.

3. How does the acceleration of a satellite change with distance from the massive object?

In general relativity, the acceleration of a satellite decreases with distance from the massive object. This is because the curvature of spacetime is weaker at larger distances, resulting in a weaker gravitational pull on the satellite. This is in contrast to Newtonian mechanics, where the acceleration would remain constant regardless of distance.

4. Can the acceleration of a satellite be affected by other massive objects in the vicinity?

Yes, in general relativity, the acceleration of a satellite can be affected by other massive objects in the vicinity. This is due to the fact that all objects with mass cause curvature in spacetime, and this curvature can affect the motion of other objects in the vicinity. This is known as the "curvature of the curvature" effect.

5. How does the acceleration of a satellite change in the presence of strong gravitational fields?

In general relativity, the acceleration of a satellite increases in the presence of strong gravitational fields. This is because the curvature of spacetime is stronger in these regions, resulting in a stronger gravitational pull on the satellite. This can be seen in situations such as near a black hole, where the acceleration can be extremely high due to the extreme curvature of spacetime.

Similar threads

  • Special and General Relativity
Replies
20
Views
1K
  • Special and General Relativity
2
Replies
47
Views
3K
  • Special and General Relativity
Replies
1
Views
648
  • Special and General Relativity
Replies
1
Views
715
  • Special and General Relativity
2
Replies
59
Views
4K
  • Special and General Relativity
Replies
4
Views
1K
  • Special and General Relativity
Replies
11
Views
353
  • Special and General Relativity
Replies
1
Views
722
  • Special and General Relativity
Replies
5
Views
1K
  • Special and General Relativity
Replies
10
Views
2K
Back
Top