Sonoma State University

Astronomy 350
J.S. Tenn

The Age of the Universe

If we assume General Relativity and the Cosmological Principle, then the age of the universe is related to three numbers (actually, three out of five). They can be

The Hubble Constant H0 = current rate of expansion

The Density Parameter Ωm = ave. density*/critical density

The (reduced) Cosmological Constant ΩΛ [Some authors call it λ, which was the symbol originally used by Einstein.]

For several decades during the middle of the twentieth century it was almost universally assumed among cosmologists that the cosmological constant must be zero. Then cosmology was "A Search for Two Numbers," the title of a famous article by Allan Sandage which appeared in Physics Today in February 1970.

If all three are known, then the age can be calculated.

If the geometry of the Universe is Euclidean (aka “flat”), then Ωm + ΩΛ = 1.

In many models, the age of the universe is close to the Hubble time, where the Hubble time TH = 1/H0.

If ΩΛ = 0 and Ωm = 1, then T0 = (2/3)TH, or the age of the Universe = 2/3 the Hubble time. (This is the critical, or just barely open Friedmann model, also called the Einstein-de Sitter model.)


If three parameters are measured then we can calculate the remaining two, the deceleration parameter q0 and the age of the Universe T0.


* This is the total density of all matter, including dark matter.

The Age of the Universe:      1     2


Please send comments, additions, corrections, and questions to
joe.tenn@sonoma.edu
JST
2008-03-19