Jump to content
Main menu
Main menu
move to sidebar
hide
Navigation
Main page
Recent changes
Random page
Help about MediaWiki
Special pages
Niidae Wiki
Search
Search
Appearance
Create account
Log in
Personal tools
Create account
Log in
Pages for logged out editors
learn more
Contributions
Talk
Editing
Hubble's law
(section)
Page
Discussion
English
Read
Edit
View history
Tools
Tools
move to sidebar
hide
Actions
Read
Edit
View history
General
What links here
Related changes
Page information
Appearance
move to sidebar
hide
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
=== Ultimate fate and age of the universe === [[Image:Friedmann universes.svg|thumb|upright=1.9|The [[age of the universe|age]] and [[ultimate fate of the universe]] can be determined by measuring the Hubble constant today and extrapolating with the observed value of the deceleration parameter, uniquely characterized by values of density parameters ({{math|Ω<sub>M</sub>}} for [[matter]] and {{math|Ω<sub>Λ</sub>}} for dark energy).<br>A '''closed universe''' with {{math|Ω<sub>M</sub> > 1}} and {{math|1= Ω<sub>Λ</sub> = 0}} comes to an end in a [[Big Crunch]] and is considerably younger than its Hubble age.<br>An '''open universe''' with {{math|Ω<sub>M</sub> ≤ 1}} and {{math|1= Ω<sub>Λ</sub> = 0}} expands forever and has an age that is closer to its Hubble age. For the accelerating universe with nonzero {{math|Ω<sub>Λ</sub>}} that we inhabit, the age of the universe is coincidentally very close to the Hubble age.]] The value of the Hubble parameter changes over time, either increasing or decreasing depending on the value of the so-called [[deceleration parameter]] {{mvar|q}}, which is defined by <math display="block">q = -\left(1+\frac{\dot H}{H^2}\right).</math> In a universe with a deceleration parameter equal to zero, it follows that {{math|1= ''H'' = 1/''t''}}, where {{mvar|t}} is the time since the Big Bang. A non-zero, time-dependent value of {{mvar|q}} simply requires [[integral|integration]] of the Friedmann equations backwards from the present time to the time when the [[particle horizon|comoving horizon]] size was zero. It was long thought that {{mvar|q}} was positive, indicating that the expansion is slowing down due to gravitational attraction. This would imply an age of the universe less than {{math|1/''H''}} (which is about 14 billion years). For instance, a value for {{mvar|q}} of 1/2 (once favoured by most theorists) would give the age of the universe as {{math|2/(3''H'')}}. The discovery in 1998 that {{mvar|q}} is apparently negative means that the universe could actually be older than {{math|1/''H''}}. However, estimates of the [[age of the universe]] are very close to {{math|1/''H''}}.
Summary:
Please note that all contributions to Niidae Wiki may be edited, altered, or removed by other contributors. If you do not want your writing to be edited mercilessly, then do not submit it here.
You are also promising us that you wrote this yourself, or copied it from a public domain or similar free resource (see
Encyclopedia:Copyrights
for details).
Do not submit copyrighted work without permission!
Cancel
Editing help
(opens in new window)
Search
Search
Editing
Hubble's law
(section)
Add topic