What the Hubble constant must be set to if Univ is flat

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Discussion Overview

The discussion centers on the Hubble constant and its implications for a flat universe, exploring theoretical and observational aspects. Participants examine the relationship between the Hubble constant, density parameters, and the Friedmann equations, while also considering the role of dark energy in determining the universe's geometry.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • One participant questions whether the Hubble constant of 70.4 km/s/Mpc is a theoretical requirement for a flat universe or an experimental measurement.
  • Another participant asserts that the Hubble constant is a measured value and cannot be derived from first principles.
  • A participant seeks clarification on the equation that determines the density parameter (omega) related to the universe's flatness.
  • Some participants reference the Friedmann equation, suggesting that for a flat universe, the equation must equal 1, and propose a relationship involving density and curvature.
  • There is a discussion about the role of dark energy, with one participant noting that changing the Hubble constant allows for adjustments in the dark energy component while maintaining a flat universe.
  • Another participant mentions that the Hubble constant must meet a specific ratio for the universe to be flat, referencing literature by Susskind.
  • Some participants highlight historical perspectives on the flatness of the universe, noting that inflation theory has changed the understanding of flat universes and their implications.
  • There is mention of the anthropic principle and its relation to the flatness problem, with a suggestion that inflation addresses many concerns without invoking anthropic reasoning.

Areas of Agreement / Disagreement

Participants express differing views on the necessity and implications of the Hubble constant for a flat universe. There is no consensus on whether the Hubble constant must take a specific value or how it interacts with dark energy in this context.

Contextual Notes

Some participants note the complexity of the relationship between the Hubble constant, density parameters, and the Friedmann equations, indicating that assumptions about these relationships may not be fully resolved.

robertjford80
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What must the Hubble constant be if the Universe is flat. At the Lamda CDM article on wiki it says 70.4 km/s mpc. I'm not sure if that's what it must be if the universe is flat or if that's what experiments have measured it to be, I'm 99% sure that it's the former but I want to be 100% sure. Also I've read the wiki article on the Hubble constant and all the various experiments that have been done to measure it so you don't need to tell me that.
 
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The Hubble constant is a measured, not theoretical value. We currently cannot derive it from first principles.
 
Could you give me some more info. I'm pretty sure what determine if the universe is flat is the density, but I forget what the equation is that determines omega.
 
Google on critical density of the universe.
 
it says a'/a is the Hubble parameter, and the friedman equation is

(8piG rho + lamda c^2)/3 = (a'^2 + kc^2)/a^2

So I would think that

(8piG rho + lamda c^2)/3 - kc^2/a^2 is what the Hubble constant would have to equal if the universe is flat, since I'm pretty sure the friedmann equation must equal 1 for a flat universe.
 
robertjford80 said:
it says a'/a is the Hubble parameter, and the friedman equation is

(8piG rho + lamda c^2)/3 = (a'^2 + kc^2)/a^2

So I would think that

(8piG rho + lamda c^2)/3 - kc^2/a^2 is what the Hubble constant would have to equal if the universe is flat, since I'm pretty sure the friedmann equation must equal 1 for a flat universe.

The parameter 'k' measures the curvature. For a flat universe, you only need k=0. The scale factor and hence the Hubble Constant at any epoch then depend on the various densities (matter, radiation, dark energy).

http://en.wikipedia.org/wiki/Friedmann_equations#The_equations
 
am I right that a'^2/a^2 is the Hubble parameter? I specifically remember reading in Sussking's the Cosmic Landscape that the Hubble constant must be a certain ratio in order for the universe to be flat. He writes:

Astronomers have been closing in on the value of the Hubble constant for almost eighty years with ever more sophisticated instruments. It now seems very unlikely that it can be small enough to allow the universe to be closed. If this were the end of the story, then we would have to conclude that the cosmic mass density was insufficient to close the universe — but we’re not done yet.
 
Last edited:
robertjford80 said:
What must the Hubble constant be if the Universe is flat. At the Lamda CDM article on wiki it says 70.4 km/s mpc.

It doesn't have to be anything in particular. Once you have dark energy, then if you change hubble's constant, then you can change the dark energy component and still end up with a flat universe.

I'm not sure if that's what it must be if the universe is flat or if that's what experiments have measured it to be, I'm 99% sure that it's the former but I want to be 100% sure.

It's a direct measurement. Also with our other observations we can tell that the universe as is flat within observational limits, but all of that are measurements.
 
robertjford80 said:
I specifically remember reading in Sussking's the Cosmic Landscape that the Hubble constant must be a certain ratio in order for the universe to be flat.

Once you add in dark energy, you have an extra variable that you can tweak.

Also in the 1970's the fact that the universe seems close to flat was considered a "problem" but flat universes pop out naturally from inflation so it's no longer considered weird or unusual that the universe is flat.

The other thing was that there's been a lot of talk about the anthropic principle, but the experience with inflation points out that one shouldn't go "anthropic" too early. In the 1970's, there were a lot of "weird coincidences" that suggested fine tuning, but inflation solved most of them without the need to go anthropic.
 

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