Is there a known parametrization for time dilation in the FLRW metric?

Click For Summary
SUMMARY

The forum discussion centers on the parametrization of time dilation within the Friedmann-Lemaître-Robertson-Walker (FLRW) metric. The user proposes a new metric format, comparing it to the Schwarzschild metric, and questions whether the new time coordinate t' represents a known parametrization. Participants clarify that the FLRW metric does not inherently reflect time dilation as seen in other metrics, and they introduce the concept of conformal time, denoted as dη, which is derived from dt' = dt/a(t). The conversation concludes with an acknowledgment that gravitational time dilation is dependent on the observer and the choice of coordinates, emphasizing the complexity of defining gravitational potential in a non-stationary universe.

PREREQUISITES
  • Understanding of the Friedmann-Lemaître-Robertson-Walker (FLRW) metric
  • Familiarity with the Schwarzschild metric and its implications for time dilation
  • Knowledge of conformal time and its mathematical representation
  • Basic concepts of general relativity and spacetime metrics
NEXT STEPS
  • Research the mathematical derivation of conformal time in cosmology
  • Explore the implications of gravitational time dilation in non-stationary spacetimes
  • Study the relationship between cosmic expansion and gravitational potential
  • Investigate alternative metrics that may reflect time dilation in cosmological contexts
USEFUL FOR

Cosmologists, theoretical physicists, and students of general relativity seeking to deepen their understanding of time dilation and metric transformations in cosmological models.

  • #31
ah gotcha, thanks for the clarification on the Milne universe. I was under the understanding that it was a matter removed model only. Not sure where I picked that mistake up from, it certainly wasn't in any of my textbooks lol
 
Physics news on Phys.org
  • #32
Peter: if something is different from the FRW metric that doesn't mean it is in conflict with GR. Your statement is in effect: there is no gravitational time dilation, because it is not in the FRW metric. That doesn't mean it does not exist. This is precisely the point a raised in my original post. I think it's not there, because we simply don't know (yet) how to calculate the cosmic potential and how it evolves. But I believe their are some clues, as I indicated before, which could help us moving forward on this, all within GR context. FRW model is not free from interrogation as long as we have no acceptable answer to what dark energy is supposed to be.
 
  • #33
Vincentius said:
if something is different from the FRW metric that doesn't mean it is in conflict with GR. Your statement is in effect: there is no gravitational time dilation, because it is not in the FRW metric. That doesn't mean it does not exist.

Ok, then show me another metric that correctly describes the universe as a whole but also allows a meaningful "gravitational time dilation" to be defined. Just waving your hands and saying "cosmic potential" doesn't mean any such metric consistent with GR does exist.

Vincentius said:
I think it's not there, because we simply don't know (yet) how to calculate the cosmic potential and how it evolves. But I believe their are some clues, as I indicated before, which could help us moving forward on this, all within GR context.

None of the clues you have mentioned so far are "within GR context"; they are either speculations on alternative theories to GR that didn't pan out, or dealing with other theoretical frameworks altogether (such as quantum mechanics).

Vincentius said:
FRW model is not free from interrogation as long as we have no acceptable answer to what dark energy is supposed to be.

Modeling dark energy in the FRW model is easy: it's a positive cosmological constant. If that's not enough for you because we don't know what microphysics produces a positive cosmological constant, that's not a problem with the FRW model; *any* large-scale model that produced the same predictions would be open to the same objection.

Also, I don't see what dark energy, or the observations that lead us to incude it in the standard cosmological model, have to do with any "cosmic potential". None of the suggestions you have made about how that might be the case were valid alternatives to the standard FRW model with a positive cosmological constant; they were misunderstandings of how the FRW model works.
 
Last edited:
  • #34
Vincentius said:
The increase of total mass within the expanding particle horizon

Btw, I haven't commented on this before: according to the best current model of the universe (the one with a positive cosmological constant, aka "dark energy"), the total mass within our particle horizon is *decreasing*, not increasing. That's because the expansion of the universe is accelerating, and the effect of the accelerating expansion (which moves matter outside the particle horizon) outweighs the effect of the increasing age of the universe (which increases the distance to the particle horizon).
 
  • #35
One quick question on a com-moving observer...

if an observer is in relative motion to the fundamental observer and to the fundamental observer the universe is homogeneous and isotropic. Am I correct in thinking that the com-moving observer would not see the universe as isotropic?
 
  • #36
Mordred said:
if an observer is in relative motion to the fundamental observer and to the fundamental observer the universe is homogeneous and isotropic. Am I correct in thinking that the com-moving observer would not see the universe as isotropic?

What you are calling the "fundamental observer" is what is usually called a "comoving observer". Those observers see the universe as homogeneous and isotropic. An observer in relative motion to the comoving observer in his vicinity will *not* see the universe as homogeneous and isotropic.
 
  • #37
thanks that's what I thought but wanted to make sure
 

Similar threads

  • · Replies 19 ·
Replies
19
Views
3K
  • · Replies 14 ·
Replies
14
Views
3K
  • · Replies 13 ·
Replies
13
Views
2K
  • · Replies 9 ·
Replies
9
Views
3K
  • · Replies 4 ·
Replies
4
Views
1K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 7 ·
Replies
7
Views
1K
  • · Replies 8 ·
Replies
8
Views
695
  • · Replies 8 ·
Replies
8
Views
4K
  • · Replies 43 ·
2
Replies
43
Views
4K