Lecture 33: EinsteinÕs
Universe
Readings: Sections 28-1 and
28-2
Key Ideas:
Cosmological Principle:
The Universe is Homogeneous and Isotropic on Large Scales
No special places or
directions
General Relativity predicts
an expanding Universe
EinsteinÕs Greatest Mistake (?)
Cosmology
Cosmology is the study
of the Universe
Physics of the
Universe
Distribution of
objects on all scales
Motions of objects
in the Universe
Evolution of the
Universe
Age, Origin, and
Fate of the Universe
The Universe in 1917
Einstein explored the
cosmological implications of General Relativity
Observational State in 1917
Kapteyn
model of the Milky Way was favored by some (but not all) astronomers.
No
agreement on the Òspiral nebulaeÓ
First
good calibrations of the P-L relations for Cepheids and RR Lyrae variables
The Cosmological Principle
The Universe is
Homogeneous and Isotropic on the Largest Scales
Critical assumption
underlying Cosmology.
Homogeneous
No special places in
the Universe
Isotropic
No special directions
Largest Scales
Average out
small-scale details
Homogeneity
When viewed on the largest
scales:
The
average density of matter is about the same in all places in the Universe
The Universe is
fairly smooth on large scales
Does not apply locally:
We see planets,
stars, galaxies in regions nearby in space
The Universe is
locally rather ÒlumpyÓ
Example from the Distribution
of Galaxies about the scales we are talking about (~100 Mpc)
Isotropy
When viewed on the largest
scales:
The Universe looks
the same to all observers
The
Universe looks the same in all directions as viewed by a particular observer
Does not apply locally
We see different
numbers of local objects in different directions.
The Dynamic Universe
Einstein applied the
Cosmological Principle to General Relativity and got a surprise:
The spacetime of the
Universe could not be static and unchanging
The Universe must either expand or contract!
In 1917, astronomers assured
him that no such general motion was observed
The Cosmological Constant
To make the Universe static,
Einstein added a new term to his equations:
The Cosmological Constant, L :
Repulsive
gravitation-like force term
Arises from empty
space
Balances the effects
of gravity
At this time, there was no
physical reason to introduce a Cosmological Constant
Cosmic Expansion
1914-22: Vesto
Slipher, Lowell Observatory measured the radial velocities of the brightest
Òspiral nebulaeÓ
Results:
21 out of 25 spirals showed a
systematic redshift
Systematic motion
away from us
Some velocities are
large: > 2000 km/sec
EinsteinÕs Greatest BlunderÉ
1920s:
DeSitter
corrects an error in EinsteinÕs math, showing that the L Universe was unstable
Friedmann
& Lemaitre showed that without L, GR predicts that
the Universe expands.
Edwin Hubble firmly
established cosmic expansion observationally in 1929.
State of the Art
EinsteinÕs guess about the
homogeneity and isotropy of the Universe was brilliant and far ahead of the
scanty empirical data of his time.
Modern observations bear out
large-scale homogeneity & isotropy on average
Large-scale galaxy
surveys
Cosmic Microwave
Background
Modern Cosmological Constant
In modern cosmology, L reappears in modified form as the Òvacuum energyÓ of space:
Quantum ground-state
of empty space
Acts as an extra
pressure on the Universe
Distinction
Actually accelerates
the expansion!
Increasing
observational evidence that L, or something very like it, may
be real