Astro 103 - Lecture 22

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A DARK MATTTER: ROTATION, MASS, AND INTERACTION



1. Rotation


Galaxy disks

Recall: not solid-body rotation

(i.e. not like a frisbee)

differential rotation


What determines orbital speed?

Mass enclosed in volume interior to orbit.


Recall Kepler's 3rd law:


(a) For Solar System, Sun is virtually ``all'' the mass

  Planets' orbital speeds decrease with orbital radius
(see lecture 15, section 3):


orbital speed 1/

(b) For a galaxy, there is substantial mass at all radii, so we expect orbital velocities of stars and gas to change differently with orbital radius in a galaxy than in the solar system.

What we observe: rotation curves

the run of orbital speed with radius in a galaxy




2. Mass


From Kepler's 3rd law:

mass (orbital radius)3 / (orbital period)2

distance3 / time2

Recall:

speed = distance / time

mass (orbital radius) x (speed)2

i.e., mass interior to orbital radius


What do we find, using rotation curves and galaxy bulk motions?

  • Rotation speed and the luminosity of a galaxy are well correlated.

    The Tully-Fisher relation

  • Galaxies weigh 1011-1012 solar masses (M)
  • Galaxy clusters weigh 1013-1015 M


There is a problem with the mass:

We count up the stars, and we don't find this much matter:

. . . not in stars,

. . . not in cold or hot gas

. . . not in dust

There must be dark halos!




3. Dark Matter


``The Dark Side ....''



What makes up dark matter?

brown dwarfs (failed stars -- Jupiters)?

cooled white dwarfs ?

cooled neutron stars?

black holes?


or ...


``Shadow'' matter

exotic fundamental particles that only interact via gravitation

- last refuge of scoundrels (theorists)


Regardless,

90% of matter in the Universe doesn't shine!


An outstanding puzzle.

How do we detect it?

(See Chap. 14.6 for one example:
gravitational micro-lensing)




4. Interactions


Glancing blows

Mergers


Computer simulations:

- initial conditions:

spatial distribution and velocities of stars and dark matter in galaxies;
bulk velocities of galaxies

- stars modeled as collisionless particles   -   why?

- pure gravitational interactions


What's missing? (dust, gas ... the sticky stuff)

Recent models include this too!

numerical simulations via Cray Supercomputers,
courtesy of Chris Mihos, Lars Hernquist and collaborators.

Results:

Tidal forces and disruption

Tidal tails

``like a hose'' ? .... not quite

If gas is included: invariably a nuclear starburst.


Galactic cannabalism:   what do you think this means?


One plausible way to transform galaxies along the Hubble Sequence:

Input: any kind of galaxy, as long as there are enough of them . . .

. . . shake well and stir . . .

giant elliptical

Only found at the centers of galaxy clusters.

Why?




Q22.1 If the rotation curve of a galaxy continues to rise at large radii, what can we infer about the distribution of galactic mass?

(a) stars are following Keplerian orbits

(b) there is substantial mass at large galactic radii

(c) all mass is contained within an interior radius

(d) there is little or no mass at large radii

(e) all mass is contained outside an interior radius


Q22.2 Galaxies exist in clusters, small groups, pairs, and isolated in space. Where would you expect to find relatively fewest spirals compared to giant ellipticals?

(a) clusters

(b) groups

(c) pairs

(d) isolated in space

(e) isolated in space and in pairs


Lectures Lecture page Astro103 page

Last updated: Aug 23, 2011 Matthew A. Bershady