Question pertaining to dark energy

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SUMMARY

The discussion centers on the concept of dark energy and its role in the expansion of the universe, particularly in relation to the Hubble Sphere. Participants clarify that while the universe appears to be accelerating, this acceleration is due to the increasing amount of space between objects rather than a uniform acceleration of all points in space. The expansion rate, denoted by the scale factor (a), is decreasing over time, but the absolute expansion continues to increase. Dark energy, characterized by a parameter w < -1/3, is essential for explaining this phenomenon, as it allows for accelerated expansion in a universe where matter alone would lead to deceleration.

PREREQUISITES
  • Understanding of cosmological concepts such as the Hubble constant and scale factor (a).
  • Familiarity with the implications of dark energy and its equation of state parameter (w).
  • Knowledge of the Big Bang theory and the dynamics of cosmic expansion.
  • Basic grasp of mathematical expressions related to cosmology, including derivatives of the scale factor.
NEXT STEPS
  • Research the implications of the cosmological constant (Λ) on the universe's expansion.
  • Study the relationship between dark energy and the Hubble constant as measured by the PLANCK mission.
  • Explore the mathematical modeling of cosmic expansion and the role of the scale factor in cosmology.
  • Investigate the differences between proper distance and scale factor in the context of expanding space.
USEFUL FOR

Astronomers, physicists, and students of cosmology who are interested in understanding the mechanisms behind the universe's expansion and the significance of dark energy in contemporary astrophysics.

  • #31
Physics1218 said:
The Friedmann equations postulate that general relativity is true.

No, they postulate that GR works within its domain of validity. There's a big difference. See below.

Physics1218 said:
If general relativity were to ever be proven incorrect, then would it be logical to say that the Friedmann equations no longer work?

No, because GR would still be the low energy classical limit of whatever theory replaced it--just as Newtonian gravity is the weak field, slow motion limit of GR. GR proved that Newtonian gravity was "incorrect" in the sense of not being exactly right, but Newtonian gravity still works fine within its domain of validity. We don't need to use GR to calculate the trajectories of artillery shells or space probes.

Similarly, the regime covered by the Friedmann equations, at least from the end of inflation (the Big Bang) to now, is well within the domain of validity of GR, i.e., the domain in which any corrections due to a more fundamental theory that incorporates quantum gravity are expected to be negligible. So any more fundamental theory won't invalidate what Chalnoth said.
 
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  • #32
Physics1218 said:
I'm sorry this is an old discussion but I was in Peru so I couldn't have internet to access it.
Where were you in Peru? I live here and even the 'nativeos' in the Andes and jungle are playing Pokemon. : )
 
  • #33
PeterDonis said:
No, because GR would still be the low energy classical limit of whatever theory replaced it--just as Newtonian gravity is the weak field, slow motion limit of GR. GR proved that Newtonian gravity was "incorrect" in the sense of not being exactly right, but Newtonian gravity still works fine within its domain of validity. We don't need to use GR to calculate the trajectories of artillery shells or space probes.
And incidentally, Newtonian gravity produces the exact same equations for expansion as General Relativity (at least as it relates to matter: Newtonian gravity only describes gravity with matter, and doesn't include gravity from other forms of energy). This is a strong indication that the Friedmann equations are a very good approximation to the behavior of our universe.

There are two places where the Friedmann equations are likely to break down:

1. The Friedmann equations assume a perfectly homogenous, isotropic universe. Our actual universe is not perfectly homogeneous or isotropic. This can lead to subtle modifications of the equations, and is a well-studied area.

2. General Relativity itself is very likely to fail at sufficiently high energy densities, which means that the Friedmann equations cannot describe the earliest beginnings of our universe. There are some that claim that this fact casts doubt on cosmic inflation (which is possible), or that quantum gravity produces a "bounce" (look up Loop Quantum Cosmology if you're curious to learn more). But in any event these only apply to the earliest beginnings of our universe, and have no effect in the later universe beyond setting up the initial conditions.
 
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  • #34
The isotropy and homogenity of the universe is observer dependent. We cannot assume otherwise based on current theory or observational evidence.
 
  • #35
Chronos said:
The isotropy and homogenity of the universe is observer dependent.

What do you mean?
 

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