BB theory and preferred frames

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SUMMARY

The discussion centers on the interpretation of the Big Bang theory and its implications regarding absolute time and preferred frames in cosmology. Participants argue that the Big Bang, as described by the Friedmann-Robertson-Walker (FRW) metric, does not imply an absolute frame due to the manifest covariance of the Einstein Field Equations (EFE). The age of the universe is defined as the proper time experienced by comoving observers, which is considered arbitrary yet well-defined. The conversation highlights the complexities of reconciling mathematical descriptions with verbal interpretations in the context of general relativity.

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  • Understanding of the Friedmann-Robertson-Walker (FRW) metric
  • Familiarity with Einstein Field Equations (EFE)
  • Knowledge of general relativity and covariance principles
  • Basic grasp of cosmological concepts such as comoving observers
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  • Study the implications of the Friedmann-Robertson-Walker (FRW) metric in cosmology
  • Explore the mathematical foundations of Einstein Field Equations (EFE)
  • Learn about the concept of comoving observers and their significance in cosmology
  • Investigate the relationship between time, singularities, and the Big Bang in general relativity
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Cosmologists, physicists, and students of general relativity who seek to deepen their understanding of the Big Bang theory and its implications for time and space in the universe.

  • #91
TrickyDicky said:
a simple way to obtain absolute motion or velocity is to have as assumption that the spatial distribution of matter be homogeneous or uniform and the same in all directions (isotropic),
That is not what is meant by "absolute velocity" in relativity. What is meant by "absolute velocity" is that the principle of relativity is violated, or in other words, that the laws of physics are different in different frames.

Mount Everest is tautologically at rest in Mount Everest's rest frame, but the laws of physics are not different in a frame where Mount Everest is moving. Therefore Mount Everests' rest frame does not constitute an absolute rest frame.

The CMB is tautologically at rest in the FRW coordinates, but the laws of physics are not different in a frame where the CMB is moving. Therefore the CMB frame does not constitute an absolute frame.

If you want to show that the CMB represents an absolute rest frame it is not sufficient to show that the CMB is at rest in some coordinate system nor even that some class of observers is at rest in that same frame, it is necessary to show that the laws of physics are different in that rest frame. That is impossible, I refer you again to post 3.
 
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  • #92
DaleSpam said:
That is not what is meant by "absolute velocity" in relativity. What is meant by "absolute velocity" is that the principle of relativity is violated, or in other words, that the laws of physics are different in different frames.
Just what I said in the last line of my post.
The laws of physics are generally considered as absolute and universal, and in that case no possible violation of the principle of relativity as you quote it s permitted by definition, turning the principle of relativity into a true tautology. To avoid ambiguities you should define clearly what a physical law is and what constitutes something that in your opinion counts as a difference in a physical law.

DaleSpam said:
Mount Everest is tautologically at rest in Mount Everest's rest frame, but the laws of physics are not different in a frame where Mount Everest is moving. Therefore Mount Everests' rest frame does not constitute an absolute rest frame.

The CMB is tautologically at rest in the FRW coordinates, but the laws of physics are not different in a frame where the CMB is moving. Therefore the CMB frame does not constitute an absolute frame.

If you want to show that the CMB represents an absolute rest frame it is not sufficient to show that the CMB is at rest in some coordinate system nor even that some class of observers is at rest in that same frame, it is necessary to show that the laws of physics are different in that rest frame. That is impossible, I refer you again to post 3.
You have some kind of obsession with tautologies, I wish you well wrt that. Also, you need to address what is actually said in the post you reply to, not what you imagine was said.
 
  • #93
TrickyDicky said:
To avoid ambiguities you should define clearly what a physical law is and what constitutes something that in your opinion counts as a difference in a physical law.
Fair enough. What would count as a difference in a physical law in different frames would be a term in the physical law which depends on the reference frame.

In the case of GR the physical law is the EFE, which contains no term depending on the reference frame. Therefore, anything which is a solution to the EFE (e.g. the FRW metric) cannot depend on the reference frame.
 
  • #94
DaleSpam said:
Fair enough. What would count as a difference in a physical law in different frames would be a term in the physical law which depends on the reference frame.

In the case of GR the physical law is the EFE, which contains no term depending on the reference frame. Therefore, anything which is a solution to the EFE (e.g. the FRW metric) cannot depend on the reference frame.
That's my point, no absolute frame is possible for the EFE solutions. Therefore no event can be assigned to a certain "absolute" date.
 
  • #95
TrickyDicky said:
That's my point, no absolute frame is possible for the EFE solutions. Therefore no event can be assigned to a certain "absolute" date.
I agree.

You can, however, adopt any convention that is convenient and use it to assign dates to events. That is all the time coordinate in the FRW metric is.
 
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