Question pertaining to dark energy

  • Context: High School 
  • Thread starter Thread starter Physics1218
  • Start date Start date
  • Tags Tags
    Dark energy Energy
Click For Summary

Discussion Overview

The discussion centers around the concept of dark energy and its role in the expansion of the universe, particularly in relation to the Hubble Sphere and the nature of cosmic acceleration. Participants explore theoretical implications, mathematical formulations, and alternative perspectives on the universe's expansion dynamics.

Discussion Character

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

Main Points Raised

  • One participant suggests that the universe's expansion is not truly accelerating in the conventional sense, proposing that while the relative rate of expansion decreases, the absolute expansion increases due to more space being created.
  • Another participant argues that without dark energy, distances between far-away objects would always decelerate, and that accelerating distances require a form of matter with an equation of state parameter \( w < -1/3 \), which is characteristic of dark energy.
  • A different viewpoint emphasizes that for accelerated expansion to occur, a positive value of \( \Omega_\Lambda \) (density parameter for dark energy) is necessary, as indicated by the second derivative of the scale factor.
  • One participant elaborates on the dynamics of expansion, explaining that in a universe devoid of matter or energy, the scale factor would grow linearly, resulting in zero acceleration, contrasting this with the effects of adding dark energy which would alter the expansion dynamics.

Areas of Agreement / Disagreement

Participants express differing views on the necessity of dark energy to explain cosmic acceleration. While some argue for its essential role, others propose alternative interpretations of the expansion dynamics that do not rely on dark energy. The discussion remains unresolved with multiple competing perspectives presented.

Contextual Notes

The discussion includes complex mathematical formulations and assumptions about the nature of the universe's contents, which are not fully resolved. The implications of different energy densities and their effects on expansion are also highlighted but not conclusively determined.

  • #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.
 
Space news on Phys.org
  • #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.
 
  • Like
Likes   Reactions: Drakkith
  • #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?
 

Similar threads

  • · Replies 17 ·
Replies
17
Views
4K
  • · Replies 33 ·
2
Replies
33
Views
7K
  • · Replies 29 ·
Replies
29
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 37 ·
2
Replies
37
Views
6K
  • · Replies 6 ·
Replies
6
Views
4K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 4 ·
Replies
4
Views
886