Astro 1050 Mon. Mar 22, 2004
|
|
|
Today: Go over exam |
|
Ch. 12: The Milky Way |
Chapter 12 The Milky Way Galaxy
|
|
|
Band of light running around sky in a
“great circle” |
|
Name from Greeks and Romans: Milky Circle, Milky Road |
|
Galileo saw it was made of thousands of
faint stars |
|
Great Circle suggests a plane of
material with us in plane (like ecliptic) |
The Milky Way (during the
Leonid Meteor Shower)
|
|
|
Milky Way made of many faint stars |
|
|
|
Bands of dark dust visible too |
|
|
|
Many types of objects (eg. O, B stars,
Hydrogen clouds) concentrated along plane of Milky Way |
Where are we within the
plane?
|
|
|
Great Circle suggests a plane of
material with us in plane (like ecliptic) |
|
|
|
Similar brightness in all directions in
plane. |
|
|
|
Does that really mean we are located in
the center? |
To sort out location will
need:
|
|
|
|
|
Bright objects visible at large
distances |
|
Objects above or below the plane – so
not as obscured |
|
|
|
Ways to measure distances to those
objects |
|
Ways to see material other than stars |
|
Gas, dust, ???, mass distribution |
|
Ways to map motion of objects in our
Galaxy |
|
|
|
Examples of other Galaxies |
|
The Shapley-Curtis debate: |
|
Are spiral nebulae external galaxies or
a type of object within our own galaxy |
Distances to the farther
stars
|
|
|
|
|
Parallax only works for nearby stars |
|
Spectroscopic “Parallax” works somewhat
further out |
|
Measure spectra and get Spectral Type
and Luminosity Class |
|
From those get Luminosity and then use
m-M to find distance |
|
Limited because need relatively bright
stars to get high resolution spectra |
|
Need another way to find M, then use
m-M to get distances |
|
|
|
Variable stars and the
Period-Luminosity relationship: |
|
Some stars vary in intrinsic brightness
with time |
|
The larger, more massive, and brighter stars vary more slowly |
|
Like the relative pitch of a large vs.
small organ pipe |
Example of a Variable
|
|
|
|
|
Cepheid Variables named after prototype
Delta Cephei |
|
RR Lyrae Variables names after
prototype RR Lyrae |
|
Related to presence of partially
ionized He at right level of star |
|
Partially ionized material can act as a
local energy source or sink |
The Instability Strip
|
|
|
If T too low partially ionized He too
deep to cause instability |
|
|
|
If T too high partially ionized He too
high to cause instability |
|
|
|
Larger stars oscillate with longer
periods |
The Period-Luminosity
Relationship
|
|
|
|
Relationship discovered by Henrietta
Leavitt in 1912 |
|
stars in Small Magellanic Cloud |
|
all at roughly same distance |
|
but didn’t have absolute M, just
apparent M |
|
need absolute M to get distances |
|
|
|
Calibrated by Harlow Shapley |
|
If you can find distance (so M-m) for
just one nearby Cepheid, you can convert Leavitt’s “m” scale to the “M” you
want. |
Calibrating the
Period-Luminosity Relationship using Proper Motion
|
|
|
|
Suppose all planes fly at 500 MPH = 733
ft/sec |
|
Observe the angle that a plane shifts
in 1 second of time |
|
|
|
|
|
A plane that moves 10 in 1
sec (900 in 90 sec) is at
42,000 ft |
|
A plane that moves 20 in 1
sec (900 in 45 sec) is at
21,000 ft |
|
|
|
Works for stars too: closer stars have faster “proper motion” |
|
Can only get average distances using
average proper motion, since any given star might be moving faster or slower
than average |
|
Harlow Shapley found 11 Cepheids with
proper motion |
|
Used average proper motion, and average
distance, to find average (M-m) |
|
Let him replace Leavitt’s relative “m”
axis with absolute “M” |
|
Now period Þ M then M-m Þ d |
Globular vs. open
clusters
|
|
|
|
Open Clusters |
|
Typically a few thousand stars |
|
Not gravitationally bound |
|
Often contain young stars |
|
Concentrated in plane of Milky Way |
|
Distributed “randomly” around the
circle of the Milky Way |
|
|
|
Globular Clusters |
|
Typically >hundred thousand stars |
|
Only contain older stars |
|
Are gravitationally bound |
|
Not strongly concentrated in plane of
Milky Way |
|
Not randomly distributed around the
circle of the Milky Way – more towards Sagittarius |
|
|
The Distribution of
Globular Clusters
|
|
|
|
Assume Globular Clusters orbit around
center of galaxy |
|
Center of Globular Cluster distribution
is 8.5 kpc in direction of Sagittarius |
|
|
|
We are about 2/3 of the way out to one
side – so “diameter” is approx. 25 kpc or 75,000 ly. |
|
|
|
Dust within the galactic plane fools us
with respect to distribution of ordinary stars |
The Shapley-Curtis
Debate: 1920
|
|
|
Are spiral nebulae really other
galaxies, or just swirling clouds of gas and dust within our own galaxy? |
|
|
|
Many spiral galaxies had much larger
radial velocities than other objects within our own galaxy |
|
|
The Andromeda Galaxy
M51: The Whirlpool Galaxy
Sensing Hydrogen Gas
|
|
|
Radio emission at 21 cm wavelength |
|
Penetrates gas and dust |
|
Requires little energy to excite |
The Structure of our
Galaxy
|
|
|
|
|
|
|
The Disk Component |
|
Stars, gas, and dust |
|
The spiral arms |
|
Size: |
|
Luminous Diameter ~ 25 kpc |
|
Thickness 300 pc – 1 kpc |
|
O stars and dust 30 pc |
|
Sunlike stars greater |
|
|
|
The Spherical Component |
|
Old Stars, but little gas or dust |
|
The Halo |
|
Globular clusters |
|
Isolated old stars |
|
red dwarfs, giants, white dwarfs |
|
The Nuclear Bulge |
Disk vs. Halo Orbits
|
|
|
|
|
|
|
The Disk Component |
|
Stars, gas, and dust |
|
The spiral arms |
|
Size: |
|
Luminous Diameter ~ 25 kpc |
|
Thickness 300 pc – 1 kpc |
|
O stars and dust smaller |
|
Sun-like stars greater |
|
|
|
The Spherical Component |
|
Old Stars, but little gas or dust |
|
The Halo |
|
Globular clusters |
|
Isolated old stars |
|
red dwarfs, giants, white dwarfs |
|
The Nuclear Bulge |
Differential Galactic
Rotation
|
|
|
Stars far from the center take longer
to orbit galaxy |
|
|
|
If all mass is at the center get
Keplerian Rotation: |
|
|
|
|
|
If M is distributed, Meffective
grows with distance, so velocity does not drop in same way |
The Galactic Rotation
Curve
|
|
|
Keplerian fall-off near center
indicates compact mass at center |
|
Flat curve throughout disk indicates
much distributed mass |
|
Lack of fall-off beyond visible “edge”
indicates “dark matter” |
Stellar Population and
Galaxy Evolution
|
|
|
|
|
“Metal” abundance during time |
|
“Metals” are elements heavier than He |
|
A given star’s atmospheric abundance is
approx. fixed at birth |
|
Interstellar metal abundance grows with
each new generation of stars |
|
Red giants and supernova eject new
heavy elements into interstellar gas |
|
Orbits during time |
|
A given star’s orbit is approx. fixed
at birth – just plows through gas |
|
Orbits of gas clouds evolve with time
since they can collide |
|
Orbits get more circular and disk-like
with time |
Traditional Model of
Galaxy Evolution
|
|
|
|
Stars are stuck with their original
orbits |
|
They plow through gas like bullets |
|
Orbits of gas can evolve |
|
Gas clouds collide and only average
motion (rotation) survives |
|
Metal abundance grows with time |
|
|
|
System starts out with little organized
motion,few metals |
|
Halo stars form at this time |
|
It contracts, velocities average out
leaving only rotation |
|
Gas collapses to form the disk |
|
Disk stars form after this has happened |
|
|
|
Some problems with traditional model |
|
Globular clusters not all same age |
|
Gap in ages between halo and disk
objects |
|
Presence of some metals in even in
oldest stars |
|
System may have formed by merger of
smaller galaxies |
|
Galactic Cannibalism |
M51: The Whirlpool Galaxy
Possible Origin of Spiral
Arms
|
|
|
|
Differential rotation smears features
out into spiral patterns |
|
|
|
But can’t be whole story: |
|
|
|
Number of times Sun has orbited the
galaxy: |
|
10 billion yr/200 million yr
= 50 times |
|
Spiral arms would have been wound up
very tightly |
|
|
|
Something must continuously rebuild
them |
Degree of
Organization
of the Spiral Arms
|
|
|
|
|
|
Different degrees of organization |
|
Grand Design
Spirals: M51 |
|
|
|
Flocculent (“wooly”) Spirals |
Degree of
Organization
of the Spiral Arms
|
|
|
|
|
|
Different degrees of organization |
|
Grand Design
Spirals: M51 |
|
|
|
Flocculent (“wooly”) Spirals |
Tracing the Spiral Arms
|
|
|
|
|
Arms NOT obvious if you look at: |
|
Old objects like the sun |
|
Arms ARE obvious if you look at: |
|
Maps of gas clouds |
|
21 cm Hydrogen |
|
Radio maps of CO |
|
Far infrared observations of dust |
|
Young stars |
|
O, B stars |
|
“HII” ionized hydrogen regions
surrounding O,B stars |
|
|
|
Clouds somehow form in arms , then
dissipate between them |
|
Short lived objects only get a short
distance from their places of birth |
|
O stars, Lifetime = few million
years, at 250 km/s Þ500 pc |
|
|
M51: The Whirlpool Galaxy
Density Wave Theory
|
|
|
|
|
SPIRAL WAVE rotates with galaxy, but
slower than individual stars |
|
Like moving traffic jam after an
accident has been cleared |
|
|
|
Gas (and stars) catch up with wave,
move through it, eventually reach front |
|
Just like cars catching up with moving
traffic jam, eventually get through it |
|
|
|
Gas is more crowded in wave – clouds
collapse to form new stars |
|
More collisions in the traffic jam |
|
|
|
There are slightly more old stars in
the arm too, because they speed up slightly coming into it and slow down
slightly moving out of it. |
|
But the best tracers are the things
that mark recent cloud collapses: O,B
stars, etc. |
|
|
Self Sustaining Star
Formation
|
|
|
Cloud collapse Þ New stars |
|
New stars Þ Supernova after few
million years |
|
Supernova Þ Shock Waves |
|
Shock Waves Þ Nearby clouds collapse |
|
|
|
Differential Rotation twists pattern
into spiral |
Two limiting cases of
spirals
|
|
|
Grand Design: Density Wave |
|
|
|
Flocculent: Self Sust. Star Form. +
Diff. Rot. |
|
|
|
In most Galaxies you have some
combination of the two |
The Nucleus of the Galaxy
|
|
|
|
Likely Black hole |
|
High velocities |
|
Large energy generation |
|
|
|
At
a=275 AU P=2.8 yr Þ 2.7 million
solar masses |
|
|
|
Radio image of Sgr A
about 3 pc across, with model of surrounding disk |
|
|
A movie of stars at the
core
|
|
|
www.mpe.mpg.de/www_ir/GC |
|
|
|
Very cool, and worth a look! |
|
|
|
This is the best evidence to date for a
massive black hole at the Galactic core.
Now essentially “proven.” |