Cosmology
GES339 Spring 2008
Syllabus
Texts: 1. Wrinkles In Time Smoot 2005
2. The First Three Minutes Weinberg 1993 (Bookstore
notes Printed 2007, same book)
3. Ned
Wright's Cosmology Tutorial
http://www.astro.ucla.edu/~wright/cosmolog.htm
4. Calibrating
the Cosmos: How Cosmology Explains Our Big Bang Universe (With Amazon
online reading upgrade) Levin 2007 (Set up an Amazon account and buy
the upgrade with the book)
II. Evaluation basis: Three exams (non-comprehensive), 5-7 homework
assignments, and
Project: a. Research paper, 10-15 pages, approved topic,
properly cited.
and b1. Individual PowerPoint
presentation, derived from the paper, defined audience, 20 min,
presented to class & to Celebration of Student Creativity &
Learning.
Or b2. Poster presentation by
1-3 students, approved topic, defined audience, presented to class and
to the annual Celebration of Student Creativity and Learning.
The course average will include 6 grades: 3 exams, 1 project, 1
assignments, + best of these.
Optional credit: You may add an incremental letter grade to your course
grade (e.g. B+ to A-) by arranging for and presenting a PowerPoint
presentation or poster to a school class in the community. You may
borrow another studentÕs presentation or poster for this.
III. Topical Outline:
1. What is Cosmology?
Readings: Smoot Ch. 1-2, 4 & Levin Ch. 1
a. Tues1/22 Definition of Universe has
changed often, but each definition meant "everything".
b. What is the universe made of?
c. Why is the sky black?
d. How big is it, or is it infinite?
e. How old is it? Can it be infinitely
old? (Steady State discussed in Smoot Ch. 4)
Thurs 1/24 Age:
19th Century estimates of the age of the earth
a. Darwin
b. Salinity of sea
c. Cooling time—thermal outflow through
the crust
d. Solar energy from gravity—Kelvin
timescale
2. Tues 1/29 Expanding
universe Readings: Smoot Ch. 3 Levin Ch. 2,3,5
a. Is the universe evolving with time? If so, what
was its past, what is its destiny?
b. Is it changing in a constant manner, or is the
change itself variable?
c. What can we know about its origin?
d. Can we ask its temperature? Is this
changing?Hubble law, Hubble radius, Hubble time
e. Velocity, Doppler shift, cosmic red shift
f. Red shift z defined
g. Expansion and temperature
3. Thurs 1/31 Distance measurement
Levin Ch. 2
a. Parallax--Hipparcos satellite
b. Discovery of universe of galaxies (Hubble; Cepheids)
c. Photometric distance measurement (Reviewed next week,
see below)
d. Cepheid distance determinations
e. Beyond Cepheid scale:
1. Expanding photospheres—Type II supernovae
2. Type Ia Supernovae
f. Results: Expansion is accelerating.
Tues. Feb 5 Distance: In-class exercise: Subtracting proper motion from
apparent
motion to get parallax;
Relationship of parallax to distance
Inverse correlation of proper motion and distance: Choosing candidates
for parallax studies.
The direction of motion of the Hyades cluster: The convergence point
The components of motion for a star whose direction (convergence point)
is known.
Ratio of tangential and radial velocity from a component triangle
Distance is known when the tangential velocity and proper motion are
known.
Distance is beyond easy parallax studies. We know with confidence the
distance of this cluster.
Thurs. Feb 7 Distance:
Standard Candles and photometric distance
measurements.:
An HR diagram (color-magnitude) reviewed.
The main sequence
The main sequence in the color-magnitude diagrams of different clusters
The different magnitudes of similar stars in different clusters are due
to differences in distance.
Is reddening a problem?
Cepheid variable in
M100
Tues. Feb 12 Guest lecture by Tom Burbine: What is a Planet? Lecture
was part of Earth Science Search for Self.
Thursday Feb. 14: Very Luminous Standard Candles Also see Feb 7
Photometric Distances
a. Type II Supernovas
b. (Expanding photospheres (review)
c. Type Ia Supernovas
d. Modern approach to Type Ia as standard candles
e. Distance vs. redshift at high z
f. Accelerating Universe!
Tues Feb. 19 Holiday
Thurs. Feb. 21 Announcement of Exam 1
Next Thurs Feb 28 Material
from beginning to Feb 14.
4. Newton, Einstein and gravity
a. Equivalence principle
b. Gravity and curved space—general relativity
c. Mass curves space-time. Matter & radiation follow
shortest curves—geodesics
d. Curved space concept:
1. Euclid's 5th axiom
2. Extending geometry by violating the
axiom:
3. Positive and negative curvature
4. Triangles
e. Some effects of the equivalence principle and curvature of space:
1. Aberration of starlight by the sun
2. Excess precession of the perihelion of Mercury
Tues. Feb 26
3. Gravitational red shift in white dwarfs
4. Einstein rings
a. Einstein Cross
b. Collection of
gravitational Lenses
c. Abell 2218: A
galaxy cluster lens
Thurs Feb 28 Exam 1 Open notes (NOT printed or photocopied!)
Two questions-Time & Distance
Tues March 4
5. Einstein universe model:
a. Gravity forbids static universe:
b. Einstein introduces cosmological
constant:
Lambda, to allow a static universe
c. Lambda represents some sort of
universal energy field, unknown to science
d. Static universe so obtained is not
stable;
also, universe is expanding.
e. Einstein called Lambda his biggest blunder.
6. Thurs Mar 6 Friedmann universe models
a. Not static—Closed, open or critical,
depending on density
b. There is a theoretical critical
density.
1. Critical density depends on
measureable physical
constants.
2. Critical density = 3*Ho2/[8*pi*G]
In
our universe it is
1.9 x 10-32 kg/m3
3. The ratio (actual
universal
density)/(critical density)
= Omega.
c. Closed Friedmann universe: Expanding
(or contracting)
but bound:
1. Density greater
than critical density
(Omega > 1)
2. Would eventually
start to contract if
expanding
3. Closed—has a finite
(increasing)
volume
4. Positive
curvature—all world-lines
intersect twice
5. The above means
this model has a
beginning and an end.
d. Open Friedmann universe: Expanding
and unbound:
1. Density less than
critical density
(Omega < 1)
2. Expands eternally
at a decreasing
rate, always above a
limiting rate.
3. Open—has infinite
volume
4. Negative
curvature—world-lines
diverge from an
intersection
5. Has a beginning
but no end
e. Critical Friedmann universe:
Expanding and unbound:
1. Density equal to
critical density
(Omega = 1)
2. Expands eternally
at a decreasing
rate, limiting rate is
zero
3. Open—has infinite
volume
4. Zero
curvature—familiar Euclidean
geometry
5. Has a beginning
but no end.
f. The actual density is a topic in itself.
7. Tues Mar 11 Mass density in the universe (Announce Exam 2-From Feb
21 to Mar 13)
(Exam 2 Topics: Gravity, Einstein &
Friedmann universe models, Density of Universe,
Age of Universe)
a. Luminous mass
b. Dynamical mass--includes dark matter
in galaxies &
clusters. Measured by gravity.
c. Baryonic mass—includes all ordinary
matter made in the
big bang. H/D ratio.
d. Theoretical total—includes enough
matter to make
space-time "flat". (Omega = 1. Reason comes later)
e. Amazing ratios of ordinary matter,
dark matter, and
energy, as we understand them.
8. Thurs Mar 13 Age of the Universe (Observational-compare with
free-expansion time)
a. Age of the oldest star clusters
(HR-diagrams
& stellar evolution)
b. Age of the oldest white dwarf stars
c. Age of the radioactive elements
9. Tues Mar 18 The hot big bang and element formation: Gamow, Alpher,
& Herman
a. Yelm
b. He production
c. Prediction of universal temperature
d. Penzias
& Wilson
e. Cosmic background radiation
f. COBE spectrum
Thurs Mar 20 Exam 2
Tues Mar 25-Thurs Mar 27 Spring Break
10. Tues April 1 The first three minutes: Modern version
a. Elementary particles- photons,
protons, neutrons,
electrons,
neutrinos & antiparticles in number equilibrium
b. As the temperature drops, the energy
to make the heavier
particles is no longer available, so annihilations become permanent and
heavier particles become rare.
d. Finally, everything is rare except
photons. That's the
beginning of the modern universe; photons are a billion times more
common than particles of matter.
e. Ultimately, temperature drops to
where D is stable. Then
all neutrons (and an equal number of protons) become bound into
He. The H-He ratio of the universe is set.
f. Density
of matter
11. Thurs April 3 The radiation horizon: T = 340,000 years
a. Universe becomes transparent
b. Ripples in the matter density are present
and potentially
visible.
c. Appearance of the horizon strongly
constrains age, total
density, and structures.
d. COBE
results: First picture of the horizon.
e. WMAP
results: The baby picture of the
universe.
12. Tues April 8 Cosmic inflation:
a. Horizon problem
b. Flatness problem
c. Smoothness problem
d. Inflation concept: The return of
Lambda with a physical
basis. Omega = 1
13. Thurs April 10 Measurement of structure: