Time according to whom, after the big bang?

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Discussion Overview

The discussion revolves around the concept of time in the context of the Big Bang and cosmological models. Participants explore the implications of relativity on time measurement and the various frames of reference used in cosmology.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants question what is meant by "time" after the Big Bang, emphasizing that time is relative and asking which frame of reference is being used.
  • One participant notes that current cosmological models suggest the universe expanded from a tiny state, with light reaching Earth that has been traveling for approximately 13.7 billion years, indicating a specific timeline since the Big Bang.
  • Another viewpoint suggests that time is discussed in the observer's frame, with some theoretical models proposing an absolute cosmological time that contradicts relativity, particularly in certain spacetimes like the RLFW model.
  • A participant challenges the idea of absolute cosmological time, arguing that relativity pertains to the motion of bodies and questioning its relevance to the timeline since the Big Bang.
  • One participant explains that in general relativity, while there are no universal frames of reference, cosmologists often use a coordinate system where the Cosmic Microwave Background (CMB) is at rest, allowing for a proper time measurement since the Big Bang.
  • Another participant elaborates that in general relativity, all reference frames are equally valid, and some spacetimes allow for a global time variable, which can be convenient for cosmological calculations.

Areas of Agreement / Disagreement

Participants express differing views on the nature of time in cosmology, with some supporting the idea of absolute cosmological time in specific models, while others emphasize the relative nature of time and the appropriateness of various reference frames. The discussion remains unresolved regarding the implications of these differing perspectives.

Contextual Notes

Participants highlight limitations in understanding time due to the dependence on specific definitions and the complexities of general relativity, which may not provide a single frame of reference applicable to all scenarios.

komodekork
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When physicist talk about time after the big bang, what do they mean? Time is relative, so which frame of reference are they talking about?

Could anyone please explain?
 
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komodekork said:
When physicist talk about time after the big bang, what do they mean? Time is relative, so which frame of reference are they talking about?

Could anyone please explain?

Current cosmological models indicate that the U was once tiny and has since expanded. Various experiments have shown that there definitely is light reaching the Earth that has been traveling for something like 13.7 billion years. and that that radiation started about 480 thousand years after the universe started not being infinitesimal. Thus the belief that the "big bang", whatever that was, happened 13.7 billion years ago (maybe plus or minus the 408 thousand, I forget).

The relative nature of time that you are talking about is a relativistic effect of motion of two objects in relation to each other. It doesn't apply to the concept that the big bang happened when it did.
 
komodekork said:
When physicist talk about time after the big bang, what do they mean? Time is relative, so which frame of reference are they talking about?

Could anyone please explain?

They are talking about time in their own frame. In a way it can't be anything else, it is the time of the observers frame. However cosmological time in some theoretical spacetimes is like an absolute cosmological time. I know this contradicts relativity but in some of these models (like the RLFW) the universe has a symmetry (killing vectors) with a constant time surface.
 
cosmik debris said:
... cosmological time in some theoretical spacetimes is like an absolute cosmological time. I know this contradicts relativity ...QUOTE]

Uh ... how is that? Relatively has to do with the relative motion of two bodies. How does time since the big bang have anything to do with that?

Thanks,

Paul
 
komodekork said:
Time is relative, so which frame of reference are they talking about?
In general, there are no frames of reference in GR that cover all of space-time (like they do in SR). However, one can usually come up with coordinate systems that cover all of space-time. Cosmologists often use a coordinate system wherein the CMB is at rest. So, the amount of time you mentioned is the amount of proper time elapsed since the big bang in the http://en.wikipedia.org/wiki/Synchronous_coordinates" in which the CMB, ideally, is a purely spacelike hypersurface.
 
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phinds said:
Uh ... how is that? Relatively has to do with the relative motion of two bodies. How does time since the big bang have anything to do with that?
No it doesn't. It has to do with reference frames. In general relativity, all reference frames are equally appropriate -- the Lorentz symmetry enjoyed by inertial observers is no longer a preferred symmetry. What cosmik is saying, however, is that some spacetimes possesses sufficient symmetry to define a global time variable (just like one does for inertial frames in special relativity). In these spacetimes, this time variable is a 'natural' choice to run a clock by. In our FRW universe, observers comoving with the expansion (at reast wrt the CMB) are in one such frame. We are (very closely) comoving observers, and so this is the clock used by modern cosmologists. But this time is still no better than any other -- one can choose whichever frame one wishes; some are simply more convenient than others. (To see what I mean by convenience, imagine using galaxy-centric coordinates to plan satellite trajectories around the Earth -- obviously one should use geocentric coordinates for such a feat.)
 
bapowell said:
No it doesn't. It has to do with reference frames. In general relativity, all reference frames are equally appropriate -- the Lorentz symmetry enjoyed by inertial observers is no longer a preferred symmetry. What cosmik is saying, however, is that some spacetimes possesses sufficient symmetry to define a global time variable (just like one does for inertial frames in special relativity). In these spacetimes, this time variable is a 'natural' choice to run a clock by. In our FRW universe, observers comoving with the expansion (at reast wrt the CMB) are in one such frame. We are (very closely) comoving observers, and so this is the clock used by modern cosmologists. But this time is still no better than any other -- one can choose whichever frame one wishes; some are simply more convenient than others. (To see what I mean by convenience, imagine using galaxy-centric coordinates to plan satellite trajectories around the Earth -- obviously one should use geocentric coordinates for such a feat.)

Yes a much better explanation.
 

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