Astro 1050 Fri. Nov. 7, 2003
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Today: Extra Credit Articles |
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Ch. 11: Neutron Stars & Black Holes |
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Ch. 12: The Milky Way |
Homework #7
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Q1 As a star runs out of hydrogen in
its core, as seen from the OUTSIDE b.becomes
cooler and more luminous. |
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Q 2 White dwarfs do not shrink
with time because
a.degenerate electron pressure does
not depend upon temperature. |
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***Q 3 Formation of the elements
heavier than Fe occured primarily c.by the r and s process of neutron
capture. |
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Q4 The Ring Nebulae has an angular
diameter of 72 arcseconds, and we estimate it is 5000 light years away. The
linear diameter is c. 1.7 light years |
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Q 5 The catastrophic explosion of
a star which occurs when its degenerate core grows larger than 1.4 solar
masses is called a b.supernova |
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Q 6 We see the Crab Nebula is
about 1.35 parsecs in radius and is expanding at a rate of 1400 km/s.
Estimate when would the supernova have exploded? d. 920 years ago. |
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Q7 Which of the below sequences
shows objects with increasing densities?
b.Red Giant -- White Dwarf --
Neutron Star -- Black Hole |
Black Holes – detection
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By definition – can’t see light from
black hole itself |
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Can see large amounts of energy
released by falling material just before it crosses RS |
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Can see motion of nearby objects caused
by gravity of black hole |
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Black Holes – detection
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Example: Like White Dwarf accretion
disk but w/ black hole instead |
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Gas from red giant companion spills
over towards black hole |
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Gas spirals in toward black hole,
through accretion disk |
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Gas will be much hotter because it
falls further, to very small RS |
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Gas will be moving at very high
velocity |
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Much faster than with white dwarf since
much closer (P2 µ a3) |
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Signature of black hole: Very high energy release, very high
velocity |
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We find MASSIVE black holes in centers
of most galaxies |
Cygnus X-1
More Cool Stuff About
Black Holes
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Time Dilation – originally “Frozen
Stars” |
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Gravitational Redshift |
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Wicked Tidal Forces |
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Hawking Radiation |
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A good online black hole FAQ: http://cosmology.berkeley.edu/Education/BHfaq.html |
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Virtual trips to neutron stars and
black holes: http://antwrp.gsfc.nasa.gov/htmltest/rjn_bht.html |
Chapter 12 The Milky Way Galaxy
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Band of light running around sky in a
“great circle” |
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Name from Greeks and Romans: Milky Circle, Milky Road |
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Galileo saw it was made of thousands of
faint stars |
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Great Circle suggests a plane of
material with us in plane (like ecliptic) |
The Milky Way (during the
Leonid Meteor Shower)
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Milky Way made of many faint stars |
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Bands of dark dust visible too |
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Many types of objects (eg. O, B stars,
Hydrogen clouds) concentrated along plane of Milky Way |
Where are we within the
plane?
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Great Circle suggests a plane of
material with us in plane (like ecliptic) |
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Similar brightness in all directions in
plane. |
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Does that really mean we are located in
the center? |
To sort out location will
need:
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Bright objects visible at large
distances |
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Objects above or below the plane – so
not as obscured |
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Ways to measure distances to those
objects |
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Ways to see material other than stars |
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Gas, dust, ???, mass distribution |
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Ways to map motion of objects in our
Galaxy |
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Examples of other Galaxies |
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The Shapley-Curtis debate: |
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Are spiral nebulae external galaxies or
a type of object within our own galaxy |
Distances to the farther
stars
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Parallax only works for nearby stars |
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Spectroscopic “Parallax” works somewhat
further out |
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Measure spectra and get Spectral Type
and Luminosity Class |
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From those get Luminosity and then use
m-M to find distance |
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Limited because need relatively bright
stars to get high resolution spectra |
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Need another way to find M, then use
m-M to get distances |
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Variable stars and the
Period-Luminosity relationship: |
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Some stars vary in intrinsic brightness
with time |
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The larger, more massive, and brighter stars vary more slowly |
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Like the relative pitch of a large vs.
small organ pipe |
Example of a Variable
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Cepheid Variables named after prototype
Delta Cephei |
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RR Lyrae Variables names after
prototype RR Lyrae |
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Related to presence of partially
ionized He at right level of star |
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Partially ionized material can act as a
local energy source or sink |
The Instability Strip
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If T too low partially ionized He too
deep to cause instability |
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If T too high partially ionized He too
high to cause instability |
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Larger stars oscillate with longer
periods |
The Period-Luminosity
Relationship
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Relationship discovered by Henrietta
Leavitt in 1912 |
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stars in Small Magellanic Cloud |
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all at roughly same distance |
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but didn’t have absolute M, just
apparent M |
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need absolute M to get distances |
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Calibrated by Harlow Shapley |
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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
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Suppose all planes fly at 500 MPH = 733
ft/sec |
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Observe the angle that a plane shifts
in 1 second of time |
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A plane that moves 10 in 1
sec (900 in 90 sec) is at
42,000 ft |
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A plane that moves 20 in 1
sec (900 in 45 sec) is at
21,000 ft |
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Works for stars too: closer stars have faster “proper motion” |
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Can only get average distances using
average proper motion, since any given star might be moving faster or slower
than average |
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Harlow Shapley found 11 Cepheids with
proper motion |
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Used average proper motion, and average
distance, to find average (M-m) |
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Let him replace Leavitt’s relative “m”
axis with absolute “M” |
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Now period Þ M then M-m Þ d |
Globular vs. open
clusters
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Open Clusters |
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Typically a few thousand stars |
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Not gravitationally bound |
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Often contain young stars |
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Concentrated in plane of Milky Way |
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Distributed “randomly” around the
circle of the Milky Way |
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Globular Clusters |
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Typically >hundred thousand stars |
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Only contain older stars |
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Are gravitationally bound |
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Not strongly concentrated in plane of
Milky Way |
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Not randomly distributed around the
circle of the Milky Way – more towards Sagittarius |
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The Distribution of
Globular Clusters
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Assume Globular Clusters orbit around
center of galaxy |
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Center of Globular Cluster distribution
is 8.5 kpc in direction of Sagittarius |
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We are about 2/3 of the way out to one
side – so “diameter” is approx. 25 kpc or 75,000 ly. |
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Dust within the galactic plane fools us
with respect to distribution of ordinary stars |
The Shapley-Curtis
Debate: 1920
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Are spiral nebulae really other
galaxies, or just swirling clouds of gas and dust within our own galaxy? |
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Many spiral galaxies had much larger
radial velocities than other objects within our own galaxy |
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The Andromeda Galaxy
M51: The Whirlpool Galaxy
Sensing Hydrogen Gas
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Radio emission at 21 cm wavelength |
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Penetrates gas and dust |
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Requires little energy to excite |
The Structure of our
Galaxy
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The Disk Component |
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Stars, gas, and dust |
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The spiral arms |
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Size: |
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Luminous Diameter ~ 25 kpc |
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Thickness 300 pc – 1 kpc |
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O stars and dust 30 pc |
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Sunlike stars greater |
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The Spherical Component |
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Old Stars, but little gas or dust |
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The Halo |
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Globular clusters |
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Isolated old stars |
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red dwarfs, giants, white dwarfs |
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The Nuclear Bulge |
Disk vs. Halo Orbits
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The Disk Component |
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Stars, gas, and dust |
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The spiral arms |
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Size: |
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Luminous Diameter ~ 25 kpc |
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Thickness 300 pc – 1 kpc |
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O stars and dust smaller |
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Sun-like stars greater |
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The Spherical Component |
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Old Stars, but little gas or dust |
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The Halo |
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Globular clusters |
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Isolated old stars |
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red dwarfs, giants, white dwarfs |
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The Nuclear Bulge |
Differential Galactic
Rotation
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Stars far from the center take longer
to orbit galaxy |
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If all mass is at the center get
Keplerian Rotation: |
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If M is distributed, Meffective
grows with distance, so velocity does not drop in same way |
The Galactic Rotation
Curve
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Keplerian fall-off near center
indicates compact mass at center |
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Flat curve throughout disk indicates
much distributed mass |
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Lack of fall-off beyond visible “edge”
indicates “dark matter” |
Stellar Population and
Galaxy Evolution
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“Metal” abundance during time |
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“Metals” are elements heavier than He |
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A given star’s atmospheric abundance is
approx. fixed at birth |
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Interstellar metal abundance grows with
each new generation of stars |
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Red giants and supernova eject new
heavy elements into interstellar gas |
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Orbits during time |
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A given star’s orbit is approx. fixed
at birth – just plows through gas |
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Orbits of gas clouds evolve with time
since they can collide |
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Orbits get more circular and disk-like
with time |
Traditional Model of
Galaxy Evolution
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Stars are stuck with their original
orbits |
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They plow through gas like bullets |
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Orbits of gas can evolve |
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Gas clouds collide and only average
motion (rotation) survives |
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Metal abundance grows with time |
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System starts out with little organized
motion,few metals |
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Halo stars form at this time |
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It contracts, velocities average out
leaving only rotation |
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Gas collapses to form the disk |
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Disk stars form after this has happened |
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Some problems with traditional model |
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Globular clusters not all same age |
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Gap in ages between halo and disk
objects |
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Presence of some metals in even in
oldest stars |
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System may have formed by merger of
smaller galaxies |
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Galactic Cannibalism |
M51: The Whirlpool Galaxy
Possible Origin of Spiral
Arms
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Differential rotation smears features
out into spiral patterns |
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But can’t be whole story: |
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Number of times Sun has orbited the
galaxy: |
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10 billion yr/200 million yr
= 50 times |
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Spiral arms would have been wound up
very tightly |
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Something must continuously rebuild
them |
Degree of
Organization
of the Spiral Arms
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Different degrees of organization |
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Grand Design
Spirals: M51 |
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Flocculent (“wooly”) Spirals |
Degree of
Organization
of the Spiral Arms
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Different degrees of organization |
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Grand Design
Spirals: M51 |
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Flocculent (“wooly”) Spirals |
Tracing the Spiral Arms
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Arms NOT obvious if you look at: |
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Old objects like the sun |
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Arms ARE obvious if you look at: |
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Maps of gas clouds |
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21 cm Hydrogen |
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Radio maps of CO |
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Far infrared observations of dust |
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Young stars |
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O, B stars |
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“HII” ionized hydrogen regions
surrounding O,B stars |
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Clouds somehow form in arms , then
dissipate between them |
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Short lived objects only get a short
distance from their places of birth |
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O stars, Lifetime = few million
years, at 250 km/s Þ500 pc |
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M51: The Whirlpool Galaxy
Density Wave Theory
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SPIRAL WAVE rotates with galaxy, but
slower than individual stars |
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Like moving traffic jam after an
accident has been cleared |
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Gas (and stars) catch up with wave,
move through it, eventually reach front |
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Just like cars catching up with moving
traffic jam, eventually get through it |
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Gas is more crowded in wave – clouds
collapse to form new stars |
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More collisions in the traffic jam |
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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. |
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But the best tracers are the things
that mark recent cloud collapses: O,B
stars, etc. |
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M51: The Whirlpool Galaxy
Self Sustaining Star
Formation
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Cloud collapse Þ New stars |
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New stars Þ Supernova after few
million years |
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Supernova Þ Shock Waves |
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Shock Waves Þ Nearby clouds collapse |
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Differential Rotation twists pattern
into spiral |
Two limiting cases of
spirals
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Grand Design: Density Wave |
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Flocculent: Self Sust. Star Form. +
Diff. Rot. |
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In most Galaxies you have some
combination of the two |
The Nucleus of the Galaxy
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Likely Black hole |
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High velocities |
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Large energy generation |
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At
a=275 AU P=2.8 yr Þ 2.7 million
solar masses |
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Radio image of Sgr A
about 3 pc across, with model of surrounding disk |
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A movie of stars at the
core
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www.mpe.mpg.de/www_ir/GC |
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Very cool, brand new, and worth a look! |
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This is the best evidence to date for a
massive black hole at the Galactic core.
Now essentially “proven.” |