Is the Hyperboloid Model Truly Homogeneous and Isotropic?

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Discussion Overview

The discussion revolves around the characteristics of the hyperboloid model in relation to the principles of homogeneity and isotropy in the universe. Participants explore the implications of different geometric models, particularly focusing on the hyperboloid compared to spherical and planar models, and whether the hyperboloid can be considered homogeneous and isotropic.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants assert that while spheres and planes are clearly homogeneous and isotropic, the hyperboloid appears to violate these principles due to the presence of a minimum point and a preferred direction.
  • Others propose that the hyperboloid can be understood in a higher-dimensional context, suggesting that when time is included, the geometry may not exhibit a saddle-point in the same way, thus challenging the initial claim of non-homogeneity.
  • A participant mentions that the hyperbolic space is characterized by constant negative curvature and lacks a preferred direction, which could support its homogeneity and isotropy.
  • Another participant emphasizes the complexity of visualizing hyperbolic space, noting that the saddle-point analogy may not be entirely accurate and that hyperbolic space has measurable properties such as diverging parallel lines and larger circumferences than expected.

Areas of Agreement / Disagreement

Participants express differing views on the homogeneity and isotropy of the hyperboloid model, with no consensus reached. Some argue for its non-homogeneous nature, while others defend its isotropic characteristics under certain conditions.

Contextual Notes

The discussion highlights the challenges in visualizing hyperbolic geometry and the potential limitations of analogies used to describe it. There are unresolved questions regarding the implications of including time in the model and the definitions of homogeneity and isotropy in this context.

quantum123
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Hi:
The principle states that : the universe is homogeneous and isotropic.
Then we have three solutions often depicted as
i) Sphere
ii) Plane
iii) Hyperboloid

I can understand that the sphere and plane is homogeneous and isotropic, but the iii) does not seems to be. There seems to be a minimum point (violates homogeneity). There seems to a preferred direction -> towards and away from the horse head if you imagine it as a horse saddle. Did I miss anything here?
 
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According to the third option, 3-dimensional space is still spherical, but not when you add the time dimension. You can imagine a similar universe as follows: take a circle, so it's a 1-dimensional universe, and let it expand with time, faster than linear. You can plot this variation in time, which gives you a horn-shaped time-space. At every point this horn is hyperboloid, because the curvature is negative in one direction and positive in another direction.

There is also a saddle-point, but where it is depends on how you hold the horn. But if you hold the time-axis vertical or horizontal, there is no saddle-point (a hyperboloid doesn't have a minimum, by the way).
 
The usual third option in the FRW geometries is a hyperbolic space with constant negative curvature at every point in space. This is a homogeneous and isotropic three-dimensional space that has no preferred direction. I am not sure whether the two-dimensional surface of a horse saddle a perfect analogy to visualize it.
 
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It's not, you have to imagine the 'saddle point' at every event in the hyperbolic space-time. Somewhat difficult to imagine!

On the other hand a hyperbolic space has circles with circumferences C > 2\piR, areas greater than \piR2 and parallel lines that diverge.

Now that is something that can be measured and therefore 'imagined'...

Garth
 
Last edited:

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