ASTR 328/438 - HW 4
1. Collapse of overdensities
Remember our discussion about the
turnaround and collapse of initial overdensities in matter-only
universes. If you have a little overdense bubble of the universe
embedded in a flat universe, show that the density of the overdensity
at maximum size is given by

where the "prime" mark means the
value
of omega0 in the overdense bubble.
2. Mass and luminosity functions
We have developed an expression
using the Press-Schecter formalism for the relative numbers of
collapsed dark matter halos as a function of mass. In the range of
masses 109 - 1012.5 Msun or so, these
represent galaxies.
We also know observationally that galaxies follow a luminosity function
(relative numbers of galaxies of a given luminosity) called the
Schecter luminosity function, with parameters L* = 2x1010
and alpha = -1.
If we assume a mass to light ratio, we can connect the two?
Make some choices for mass-to-light ratio (remember this is total
mass-to-light ratio, not stellar mass-to-light ratio) and see if you
can make the PS mass function and the Schecter luminosity function
match up. Explain why you chose those mass-to-light ratios -- are they
(somewhat) physically motivated?
Only worry about mass ranges for galaxies (where this discussion is
applicable), and remember that you are allowed to shift the curves up
and down arbitrarily to make them match.
If you can succeed in matching them up with a single mass-to-light
ratio, that suggests that star formation history is similar for all
galaxies regardless of mass. If you can't succeed in matching them up
with a single mass-to-light ratio, that argues that star formation is
different in low and high mass galaxies. What do your tests suggest? If
it fits across all masses, what is the mass-to-light ratio that works,
and does that make sense physically? If it doesn't work, what would you
have to do to make it work, and what does that suggest physically?
3. Baryon Budgeting
Use the literature to get
estimates of the following for the Coma cluster:
- Total mass
- Mass of X-ray emitting gas
- Mass of stars
From this calculate a local value of the baryon/dark matter ratio
in Coma. Then figure out what you would expect cosmologically given our
discussions of OmegaB and OmegaM. Do these two
numbers match? If not, give some physical reasons why they might not
match.
4. Group Project: Cosmic Flows
We are going to study the motion
of the local group on large scales. This involves two conceptual steps:
finding peculiar velocities for clusters of galaxies, and then, once a
sample is cluster peculiar velocities is built up, solving for the
motion. So we'll do this in steps.
First, get a feel for finding peculiar velocities by the following
exercises:
- Find the peculiar velocity of a distant (ie > 50 Mpc)
cluster of galaxies not named Coma using Tully-Fisher.
- Find the peculiar velocity of a distant (ie > 50 Mpc)
cluster of galaxies not named Coma using Fundamental Plane / Dn-sigma.
OK, now you have some data. Obviously two data points isn't
enough. Now go out and grab somebody else's big catalog of cluster
peculiar velocities so you have a big dataset. Then using their data
plus yours, solve for the peculiar velocity (speed and direction) of
the local group, using the handout from Mihalas and Binney to show you
the way. Compare the velocity you get to the local group's velocity
with respect to the microwave background. Comment on differences.