Coordinate dependence of recession velocities

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Discussion Overview

The discussion centers on the coordinate dependence of recession velocities of distant galaxies, particularly in the context of FRW (Friedmann-Robertson-Walker) coordinates and their implications in both curved and flat spacetimes, including the Milne universe. Participants explore the nature of coordinate choices in relation to superluminal velocities and the properties of different spacetime geometries.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants assert that superluminal recession velocities are a result of the choice of FRW coordinates, questioning whether other coordinate systems could be applicable.
  • Others argue that in curved spacetime, global coordinate choices will exhibit counterintuitive properties, suggesting that coordinate speeds do not have physical meaning.
  • It is proposed that FRW coordinates are compelling due to their alignment with the symmetries of specific curved spacetimes, while other spacetimes may necessitate different coordinate choices.
  • Participants discuss the nature of velocities in the Milne universe, with some claiming that recession velocities are not superluminal in flat spacetime, while others challenge this view by highlighting the superluminal nature of coordinate velocities in FRW coordinates.
  • There is contention regarding the implications of coordinate velocities in the Milne universe, with some insisting that Minkowski spacetime does not exhibit superluminal velocities, while others argue that coordinate-dependent velocities can still be superluminal in certain contexts.
  • Some participants emphasize the importance of mathematical rigor in understanding these concepts, suggesting that assumptions should be validated through calculations.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the implications of coordinate choices on recession velocities, particularly in the context of FRW and Milne coordinates. The discussion remains unresolved, with no consensus on the correctness of the various claims made.

Contextual Notes

Limitations include the dependence on specific coordinate choices and the unresolved nature of the mathematical implications of these choices in both curved and flat spacetimes.

timmdeeg
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Superluminal recession velocities of far away galaxies are due to the choice of FRW-coordinates. As @Ibix said here #71 "The key point, in this context, is that you will never see these galaxies overtake a light pulse."

But is there any other choice? Riemann normal coordinates don't seem to be the right answer because - if I understand it correctly - they describe the neighborhood of the origin and are thus not applicable globally.

Is the choice of FRW-coordinates compelling because curved spacetime can not be transformed away?
 
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timmdeeg said:
is there any other choice?

It depends on what you mean by "other choice".

In a curved spacetime, any global choice of coordinates will have counterintuitive properties like coordinate speeds not always obeying the "nothing goes faster than the speed of light" rule. That is just a manifestation of the fact that that rule is not valid for curved spacetimes. You have to use the more general form of the rule, which is "everything moves within the local light cones"--or, as @Ibix said, nothing can overtake a light pulse. Coordinate speeds have no physical meaning anyway, so fixating on them is a mistake.
 
timmdeeg said:
Is the choice of FRW-coordinates compelling because curved spacetime can not be transformed away?

No. FRW coordinates are a compelling choice because they match the particular symmetries of this particular family of curved spacetimes. Different curved spacetimes with different symmetries make different coordinate choices compelling--for example, Schwarzschild coordinates in Schwarzschild spacetime.
 
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timmdeeg said:
Superluminal recession velocities of far away galaxies are due to the choice of FRW-coordinates.

What can be said about "velocities" in FRW (like) coordinates in Minkowski spacetime (the Milne Universe)?
 
George Jones said:
What can be said about "velocities" in FRW (like) coordinates in Minkowski spacetime (the Milne Universe)?
You mean the "empty universe". In flat spacetime (the Milne universe) special relativity holds globally. So recession velocities aren't superluminal.

@PeterDonis thanks for your answers, I will come back to that tomorrow.
 
timmdeeg said:
You mean the "empty universe". In flat spacetime (the Milne universe) special relativity holds globally. So recession velocities aren't superluminal.
This was not the question. The question was about coordinate velocities in Milne coordinates.
 
timmdeeg said:
In flat spacetime (the Milne universe) special relativity holds globally. So recession velocities aren't superluminal.

This is not correct. As @Orodruin said, you should look at the coordinate velocities in FRW coordinates for this case (what @Orodruin called "Milne coordinates"). You will find that those coordinate velocities are superluminal for comoving objects sufficiently far apart.
 
PeterDonis said:
This is not correct.
I am not sure why this is not correct. I've been talking about the Milne universe and thus about Minkowski spacetime with non-superluminal velocities, see The Milne universe occurs ... in flat Minkowski spacetime.

This example is very illustrative as it reveals coordinate dependent velocities in the case of the empty universe. The OP refers to curved spacetime though.
 
timmdeeg said:
I am not sure why this is not correct. I've been talking about the Milne universe and thus about Minkowski spacetime with non-superluminal velocities, see The Milne universe occurs ... in flat Minkowski spacetime.
The issue was the superluminality of the coordinate speed of the separation in FRW coordinates. This is also the case for Milne coordinates. Just as in Minkowski space, parallel transport of a local (subluminal) 4-velocity between any events in the general RW spacetime will result in a (subluminal) 4-velocity at the new point.
 
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  • #10
PeterDonis said:
No. FRW coordinates are a compelling choice because they match the particular symmetries of this particular family of curved spacetimes. Different curved spacetimes with different symmetries make different coordinate choices compelling--for example, Schwarzschild coordinates in Schwarzschild spacetime.
But isn't the difference that for Schwarzschild geometry one can use Schwarzschild coordinates, Kruskal-Szekeres coordinates and others, whereas the geometry of our universe permits the choice of coordinates only the empty case?
 
  • #11
timmdeeg said:
I am not sure why this is not correct.

That is because you are guessing instead of doing the math. Do the math.

timmdeeg said:
I've been talking about the Milne universe

Yes, we know that. We know what the Milne universe is.

timmdeeg said:
and thus about Minkowski spacetime with non-superluminal velocities

Minkowsi spacetime has non-superluminal coordinate velocities in standard Minkowski inertial coordinates. It does not have all non-superluminal coordinate velocities in FRW coordinates. Do the math and see.

timmdeeg said:
This example is very illustrative as it reveals coordinate dependent velocities in the case of the empty universe.

Exactly: coordinate dependent velocities. Do you understand what that means?

timmdeeg said:
The OP refers to curved spacetime though.

You think it does, but you are wrong, since the Milne universe is precisely a non-curved spacetime example of the phenomenon you describe. That is what we are trying to tell you.
 
  • #12
timmdeeg said:
the geometry of our universe permits the choice of coordinates only the empty case?

No. There are an infinite number of possible coordinate charts you can choose on any spacetime.
 
  • #13
@PeterDonis thanks for you very instructive answers and encouraging remarks.
 
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