Cosmological Principle: Finite or Finiteless Universe?

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Discussion Overview

The discussion revolves around the implications of the Cosmological Principle on the nature of the universe, specifically whether it can be finite or must be finiteless. Participants explore the relationship between the principle's assumptions of homogeneity and isotropy and the existence of boundaries in the universe, as well as the implications for the Robertson-Walker metric and the scale factor R(t).

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants argue that the Cosmological Principle implies a finiteless universe, questioning how a boundary could coexist with the principle's requirements for homogeneity and isotropy.
  • Others clarify that R(t) in the Robertson-Walker metric represents the scale factor rather than a physical radius, suggesting that expansion does not necessitate a boundary.
  • A participant points out that a finite universe could exist without boundaries, citing examples such as a closed universe (k = 1) or a flat universe with a multiply-connected topology.
  • One participant expresses uncertainty about how to prove the proposition regarding the universe's finiteness or infiniteness, noting that current data is indecisive.

Areas of Agreement / Disagreement

Participants express differing views on whether the universe can be finite while adhering to the Cosmological Principle. There is no consensus on the implications of boundaries in relation to the principle, and the discussion remains unresolved.

Contextual Notes

Participants highlight limitations in current data and the complexity of definitions regarding the universe's topology and curvature, which may affect interpretations of the Cosmological Principle.

touqra
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The Cosmological Principle says that the universe is homogenous and isotropic. Doesn't this imply that our universe cannot be in finite size, but is finiteless? If it has a boundary, how can then the cosmological principle still be true for those heavenly bodies residing at the boundary of the universe?

If the universe has no boundary, how can we have R(t), where R is the radius of the universe in the Robertson-Walker metric? Or even in determining the future of our universe, for the different k values, 0, 1, and -1, eg, expanding forever, or Big Crunch etc.?
 
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touqra said:
If the universe has no boundary, how can we have R(t), where R is the radius of the universe in the Robertson-Walker metric? Or even in determining the future of our universe, for the different k values, 0, 1, and -1, eg, expanding forever, or Big Crunch etc.?
R is not the radius of a universe ball taken from some center, it is the radius of curvature; ie., it would be the radius of the 3-sphere if the universe was a 3-sphere (spheres don't have boundaries). Similarly, expansion/contraction does not necessitate a boundary. Ie., increasing/decreasing the radius of a sphere causes the points of the sphere to move away/towards each other isotropically. The singularity referred to in the Big Bang is not the point singularity of a black hole; it is rather a singularity, "everywhere".
 
Last edited:
Thanks for the reply.

But, I still have a question unanswered:

The Cosmological Principle says that the universe is homogenous and isotropic. Doesn't this imply that our universe cannot be in finite size, but is finiteless? If it has a boundary, how can then the cosmological principle still be true for those heavenly bodies residing at the boundary of the universe?
 
How would you prove that proposition? Current data is indecisive.
 
touqra said:
The Cosmological Principle says that the universe is homogenous and isotropic. Doesn't this imply that our universe cannot be in finite size, but is finiteless? If it has a boundary, how can then the cosmological principle still be true for those heavenly bodies residing at the boundary of the universe?

You are right and wrong. You are right in saying that the cosmological principle can't apply in a universe with a boundary. You are wrong in saying that a cosmological universe can't apply in a finite universe. Why? Because a finite universe does not necessarily have a boundary. A closed universe (k = 1) is one example of this. A flat universe (k = 0) with a multiply-connected topology (e.g. a flat torus, T^2) is another example.

If the universe has no boundary, how can we have R(t), where R is the radius of the universe in the Robertson-Walker metric? Or even in determining the future of our universe, for the different k values, 0, 1, and -1, eg, expanding forever, or Big Crunch etc.?

R(t) in the Robertson-Walker metric is not the radius of the universe. It is the scale factor. It is a measure of how distances scale with time in an expanding (or contracting) universe. If R(t1)/R(t0) = 2, where t1 is some time later than t0, and you have two galaxies separated by 100 million light years at t = t0, and both have negligible peculiar motions, then these two galaxies will be separated by 200 million light years at t = t1.
 

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