GALAXIES
Review
 The distance of Andromeda
 Island Universes
 Galactic Coordinate System
 The location of the sun in MilkyWay
(Shapely)
 Oort’s method and mapping the Milky Way
 Proper motion
 The rotation curve of MilkyWay
 Metallicity
 Stellar populations
 The distribution of stars in MilkyWay
 The Formation of a galaxy
 Classification of galaxies
Test
Where are these objects located in sky/Milky Way?
NGC 6946 and NGC
6939
Face on spiral galaxy
Open Cluster
In Cepheous
Messier Marathon
Supernova in NGC 6946
Test
What type this supernova is?
What population the originating star was?
Normal Galaxies
Spirals Ellipticals
Morphology Disk + bulge,
Spiral arms
All bulge
Stellar population Young and old stars Old stars only
Interstellar material Present Virtually none
Star Formation Present None
Kinematics Disk rotating, Bulge and
halo have random 3-D
orbits
Little rotation, mostly
random 3-D orbits
Spiral ArmsWinding Problem
Spiral Pattern
 1960 Lin-Shu theory of density waves
 Spiral arms are waves of excess density
 Stars are crowded together temporarily
 Cosmic traffic jam
 Stars enter and exit the wave just as cars
enter and exit a jam
Precession of orbits
No Wave
Fixed frame Rotating frame
Aligned Orbits
Bar Wave Spiral Wave
Resonances
 Spiral arms are
instance
representation of
waves
 Corotation circle
 ωorbital* = ωwave
 Lindblad resonances
 Particular point in
orbit
Bars
 Computer simulations predicts:
 Bars are formed besides spiral arms
 Resonance
 Bars transfer the lost angular momentum
 Bars destroy themselves
Question
 We know bars are formed necessarily
 Bars destroy themselves
 And 75% of spiral galaxies are barred spirals.
How?
Summary
 Galaxies are not born with a given shape
(barred or unbarred)
 A typical spiral galaxy spend ¾ of its life time
barred
Galactic Center
 Evidences of stellar formation in the last 50
million years
 ISM orbits the center in a orbit with inner
radius of 2pc
 Strong magnetic field (milli-Gauss)
 Compact radio source (Sgr A)
 High radial velocities and proper motion
 Existence of a large unseen, compact object
Problem
 We can observe the center of the MilkyWay
in infrared light
 We predict there are hot, massive stars there
 We cannot distinguish the exact spectral type
of the stars in the center of the MilkyWay
 Why?
Problem
 Find the mass of Sgr A
 A star identified rotating SgrA, with orbital
velocity = 1000 km/sec that lies 0.01 pc from
SgrA.
Problem
 Is galaxy a Keplerian system?
 VLBA measurements of SgrA set limits of
~3AU for the size of SgrA:What is SgrA?
VLBA
Vary Long Baseline Array
Rotation
in
Elliptical
Galaxies
and Bulges
of Spirals
 Stars have random
velocities in 3D
 Δλ = Observed size of a spectral line
 σ =Velocity dispersion
 Faber-Jackson Relation
Gravitational binding energy
(potential of a mass distribution of
radius R and mass M)
Kinetic energy
Virial theorem
 Faber-Jackson Relation
Assumption
Luminosity and the velocity dispersion in a elliptical
galaxy are related.
 Faber-Jackson Relation
Assumption
Luminosity and the velocity dispersion in a elliptical
galaxy are related.
Tully-Fisher Relation
 Luminosity of spiral galaxies are related to
their velocity width.
 Standard candle
Tully-
Fisher
Relation
as
Standard
Candles
Luminosity
 Elliptical galaxies:
 Ie : surface brightness at re
 re : radius enclosing 50% of flux
Luminosity
 Spiral galaxies:
 I0 : central surface brightness
 r0 : disk scale length
Problem
 A star is orbiting around a galaxy.
Orbital velocity = v
Distance from the center of the galaxy = R
Find the mass within R.
Evidences
 1933: Fritz Zwicky studied the motions of 7
galaxies in a group in Coma Cluster
 Dynamic Mass: mass calculated using
gravitation laws and the velocity dispersions
 Dynamic Mass / Luminosity Mass > 400
 Clusters: temporal structures
Evidences
 1970:Vera Rubin noted rotation curve of
spiral galaxies (dynamic vs. luminous mass)
 Dynamic mass is measured using
gravitational influences
 Gravitation laws are false! Or luminous mass
is not accurate
 There are large amount of hidden mass
Dark Matter
 Dark matter is not significant in Solar System
 Dark matter surrounds spirals and ellipticals’
 Dark matter is significant in galaxy clusters
Dark matter was not required if
 Large structures (eg. Galaxies) weren’t bound
systems
(galaxies are bound systems at least in a time
equals to the age of the universe)
 Gravity laws were wrong in large scales
Candidates for Dark Matter
 Neutrinos or other exotic sub-atomic
particles
 Byronic matter
Sub-atomic particles
 Widely distributed
 No interaction with regular (baryonic) matter
 Absent in solar neighborhood
 Axions: required to explain some aspects of
the strong nuclear force
 Neutrinos
 Supersymmetric particles
 WIMPS (Weakly Interacting Massive
Particles), CHAMPS, etc.
 Baryonic Matter: not luminous.
ancient white dwarfs, brown dwarfs, chunks
of cold matter significantly larger than the
wavelength of visible light, small black holes
What have been found
 No axions orWIMP was found.
 Neutrinos may have non-zero mass.
 But the large amount of massive neutrinos
arise other problems.
 MACHO: Massive Compact Halo Objects
 brown dwarfs or dim white dwarfs or other low
mass stars
 MilkyWay halo has 50% MACHOs.With masses
around 0.1 to 0.5% of the mass of the sun.
Galaxies
Galaxies

Galaxies

  • 1.
  • 2.
    Review  The distanceof Andromeda  Island Universes  Galactic Coordinate System  The location of the sun in MilkyWay (Shapely)  Oort’s method and mapping the Milky Way  Proper motion
  • 3.
     The rotationcurve of MilkyWay  Metallicity  Stellar populations  The distribution of stars in MilkyWay  The Formation of a galaxy  Classification of galaxies
  • 4.
    Test Where are theseobjects located in sky/Milky Way?
  • 5.
    NGC 6946 andNGC 6939 Face on spiral galaxy Open Cluster In Cepheous Messier Marathon
  • 6.
  • 7.
    Test What type thissupernova is? What population the originating star was?
  • 8.
    Normal Galaxies Spirals Ellipticals MorphologyDisk + bulge, Spiral arms All bulge Stellar population Young and old stars Old stars only Interstellar material Present Virtually none Star Formation Present None Kinematics Disk rotating, Bulge and halo have random 3-D orbits Little rotation, mostly random 3-D orbits
  • 9.
  • 10.
    Spiral Pattern  1960Lin-Shu theory of density waves  Spiral arms are waves of excess density  Stars are crowded together temporarily  Cosmic traffic jam  Stars enter and exit the wave just as cars enter and exit a jam
  • 11.
  • 12.
    No Wave Fixed frameRotating frame
  • 13.
  • 14.
    Resonances  Spiral armsare instance representation of waves  Corotation circle  ωorbital* = ωwave  Lindblad resonances  Particular point in orbit
  • 15.
    Bars  Computer simulationspredicts:  Bars are formed besides spiral arms  Resonance  Bars transfer the lost angular momentum  Bars destroy themselves
  • 16.
    Question  We knowbars are formed necessarily  Bars destroy themselves  And 75% of spiral galaxies are barred spirals. How?
  • 18.
    Summary  Galaxies arenot born with a given shape (barred or unbarred)  A typical spiral galaxy spend ¾ of its life time barred
  • 19.
    Galactic Center  Evidencesof stellar formation in the last 50 million years  ISM orbits the center in a orbit with inner radius of 2pc  Strong magnetic field (milli-Gauss)  Compact radio source (Sgr A)  High radial velocities and proper motion  Existence of a large unseen, compact object
  • 20.
    Problem  We canobserve the center of the MilkyWay in infrared light  We predict there are hot, massive stars there  We cannot distinguish the exact spectral type of the stars in the center of the MilkyWay  Why?
  • 21.
    Problem  Find themass of Sgr A  A star identified rotating SgrA, with orbital velocity = 1000 km/sec that lies 0.01 pc from SgrA.
  • 22.
    Problem  Is galaxya Keplerian system?  VLBA measurements of SgrA set limits of ~3AU for the size of SgrA:What is SgrA?
  • 23.
  • 24.
  • 25.
     Δλ =Observed size of a spectral line  σ =Velocity dispersion
  • 26.
     Faber-Jackson Relation Gravitationalbinding energy (potential of a mass distribution of radius R and mass M) Kinetic energy Virial theorem
  • 27.
     Faber-Jackson Relation Assumption Luminosityand the velocity dispersion in a elliptical galaxy are related.
  • 28.
     Faber-Jackson Relation Assumption Luminosityand the velocity dispersion in a elliptical galaxy are related.
  • 29.
    Tully-Fisher Relation  Luminosityof spiral galaxies are related to their velocity width.  Standard candle
  • 30.
  • 31.
    Luminosity  Elliptical galaxies: Ie : surface brightness at re  re : radius enclosing 50% of flux
  • 32.
    Luminosity  Spiral galaxies: I0 : central surface brightness  r0 : disk scale length
  • 33.
    Problem  A staris orbiting around a galaxy. Orbital velocity = v Distance from the center of the galaxy = R Find the mass within R.
  • 35.
    Evidences  1933: FritzZwicky studied the motions of 7 galaxies in a group in Coma Cluster  Dynamic Mass: mass calculated using gravitation laws and the velocity dispersions  Dynamic Mass / Luminosity Mass > 400  Clusters: temporal structures
  • 36.
    Evidences  1970:Vera Rubinnoted rotation curve of spiral galaxies (dynamic vs. luminous mass)  Dynamic mass is measured using gravitational influences  Gravitation laws are false! Or luminous mass is not accurate  There are large amount of hidden mass
  • 38.
    Dark Matter  Darkmatter is not significant in Solar System  Dark matter surrounds spirals and ellipticals’  Dark matter is significant in galaxy clusters
  • 39.
    Dark matter wasnot required if  Large structures (eg. Galaxies) weren’t bound systems (galaxies are bound systems at least in a time equals to the age of the universe)  Gravity laws were wrong in large scales
  • 40.
    Candidates for DarkMatter  Neutrinos or other exotic sub-atomic particles  Byronic matter
  • 41.
    Sub-atomic particles  Widelydistributed  No interaction with regular (baryonic) matter  Absent in solar neighborhood
  • 42.
     Axions: requiredto explain some aspects of the strong nuclear force  Neutrinos  Supersymmetric particles  WIMPS (Weakly Interacting Massive Particles), CHAMPS, etc.
  • 43.
     Baryonic Matter:not luminous. ancient white dwarfs, brown dwarfs, chunks of cold matter significantly larger than the wavelength of visible light, small black holes
  • 44.
    What have beenfound  No axions orWIMP was found.  Neutrinos may have non-zero mass.  But the large amount of massive neutrinos arise other problems.  MACHO: Massive Compact Halo Objects  brown dwarfs or dim white dwarfs or other low mass stars  MilkyWay halo has 50% MACHOs.With masses around 0.1 to 0.5% of the mass of the sun.

Editor's Notes

  • #5 Astronomy Avoidance Zone Shapley Where does the galaxy located in the universe?
  • #8 Type Ia Globular Clusters and galaxy halo Population II, low amount of metals
  • #12 Mercury, Lunar, Solar/Lunar eclipses Climate
  • #15 Both speeds are clockwise in this example Inner region faster (hit wave) Outer slower (hit by wave)
  • #16 Lost angular momentum, from the matter that falls into the central black hole
  • #21 Because the peak wavelength for these stars is at 5.1x106/T=5.1x106 nmºK/30000ºK= 170nm, a much shorter wavelength than even J at 1.25µm=1250nm. Blackbodies at wavelengths much longer than their peaks all asymptote to the same form so the infrared won't identify these stars easily.
  • #30 Luminosity is related to observable apparent brightness and distance.
  • #31 Luminosity is related to observable apparent brightness and distance.
  • #32 Luminosity is related to observable apparent brightness and distance.
  • #33 Luminosity is related to observable apparent brightness and distance.
  • #34 Luminosity is related to observable apparent brightness and distance.
  • #35 Luminosity is related to observable apparent brightness and distance.