What is conformal time?

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Discussion Overview

The discussion revolves around the concept of conformal time in cosmology, particularly in relation to the expansion of the universe and the calculation of distances in an expanding universe. Participants explore the implications of conformal time for understanding the particle horizon and the observable universe.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants question why the age of the universe multiplied by the speed of light does not yield the current distance to the particle horizon, citing the expansion of the universe as a key factor.
  • One participant suggests that conformal time could be understood as the time it would take for light to reach us if the universe were static, although this interpretation is contested.
  • Another participant emphasizes that the scale factor of the universe varies over time, which complicates calculations and justifies the use of comoving distance and conformal time.
  • Several participants reference figures from cosmological literature to illustrate how conformal time is defined and its relationship to light travel in an expanding universe.
  • There is a discussion about the implications of recession velocity on the interpretation of conformal time, with differing views on how this affects the understanding of distances in cosmology.

Areas of Agreement / Disagreement

Participants express differing interpretations of conformal time and its implications for understanding the universe's expansion. There is no consensus on a single definition or interpretation, and the discussion remains unresolved regarding the nuances of conformal time.

Contextual Notes

Participants reference specific figures and models from cosmological studies, indicating that their understanding of conformal time is dependent on these visual aids and the definitions used in those contexts. The discussion highlights the complexity of the topic and the need for careful consideration of assumptions in cosmological models.

Dark85
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TL;DR
The wikipedia pages for the Particle horizon of the universe has the following statement:

"Due to the expansion of the universe, it is not simply the age of the universe times the speed of light (approximately 13.8 billion light-years), but rather the speed of light times the conformal time."

What is conformal time in simple terms? Why can't we just multiply the age of the universe times the speed of light?
The wikipedia pages for the Particle horizon of the universe has the following statement:

"Due to the expansion of the universe, it is not simply the age of the universe times the speed of light (approximately 13.8 billion light-years), but rather the speed of light times the conformal time."

What is conformal time in simple terms? Why can't we just multiply the age of the universe times the speed of light?
 
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Dark85 said:
Why can't we just multiply the age of the universe times the speed of light?
Please stop and think about what "expansion" means. The galaxies at the edge of our observable universe emitted the light that we now see some 13+ billion years ago, BUT ... they have been moving away from us for all of those years and are now about 50 billion light years away.
 
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Dark85 said:
What is conformal time in simple terms?
See figure 1 in Taylor and Lineweaver, which is a distance-vs-time chart of the universe.

The top chart has a horizontal scale in units of measured distance and the vertical scale in units of wristwatch time for an observer in a galaxy. Notice the particle horizon is not a straight line, which is why you can't use your linear assumption.

The middle chart is the same thing but rescaled into comoving coordinates - so the horizontal scale is stretched by different amounts at different times so that galaxies have constant coordinates. This is why the fine grey lines representing galaxies in this diagram are vertical while they were curved away from our location (the origin of coordinates) in the first one.

The bottom chart is the same as the middle one except that the vertical scale has been stretched so that light travels on 45° lines. This is the definition of conformal time - it is a rescaled time coordinate chosen so that for light the comoving coordinate distance travelled per unit conformal time is constant.
 
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The point is that the scale factor of the universe is time varying in a non-trivial manner. Sometimes maths is easier if we move that complexity into the definition of our coordinates, and in those cases we use comoving distance and conformal time.
 
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I think conformal time could be interpreted as the time it would have taken for light to reach us if the universe were static, that is, if throughout its history the galaxies had been at the same distance from us as they are currently.
 
Jaime Rudas said:
I think conformal time could be interpreted as the time it would have taken for light to reach us if the universe were static, that is, if throughout its history the galaxies had been at the same distance from us as they are currently.
Hm ... given that the recession velocity varies with distance, I don't think so.
 
Dark85 said:
Why can't we just multiply the age of the universe times the speed of light?
The particle horizon refers to the current distance of the most distant (comoving) object that we can, in principle, observe today. The light coming from that object was emitted 13.8 billion years ago and, since the speed of light is constant, we can conclude that this light has traveled 13.8 billion light-years. However, during those 13.8 billion years, the universe has expanded so much that the object that emitted that light (and, therefore, the particle horizon) is currently about 46.5 billion light-years away.
 
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phinds said:
Hm ... given that the recession velocity varies with distance, I don't think so.
I don't see how this affects what I proposed. However, if you look at the bottom panel of Figure 1 in Davis & Lineweaver (which is where conformal time is plotted), you can see that the light cone is a straight line, that is, compatible with the Minkowski metric.
 
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Jaime Rudas said:
I don't see how this affects what I proposed. However, if you look at the bottom panel of Figure 1 in Davis & Lineweaver (which is where conformal time is plotted), you can see that the light cone is a straight line, that is, compatible with the Minkowski metric.
Well, I was taking your statement
Jaime Rudas said:
I think conformal time could be interpreted as the time it would have taken for light to reach us if the universe were static, that is, if throughout its history the galaxies had been at the same distance from us as they are currently.
to mean that the time would be equivalent to a static universe where the edge of the O.U. was ~50billion LY away, implying a 50billion year age. Guess I interpreted it wrong.
 
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phinds said:
Well, I was taking your statement

to mean that the time would be equivalent to a static universe where the edge of the O.U. was ~50billion LY away, implying a 50billion year age. Guess I interpreted it wrong.
Yes, that's more or less it: conformal time would be equivalent to the time in the last 46.5 billion years of a static universe, as shown in the bottom panel of Figure 1.
 
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