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AS1001:Extra-Galactic Astronomy Lecture 3: Galaxy Fundamentals

AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

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Page 1: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

AS1001:Extra-Galactic Astronomy

Lecture 3: Galaxy Fundamentals

Page 2: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

Galaxy Fundamentals

•  How many stars are in a galaxy ? •  How did galaxies form ? •  How many galaxies are there ? •  How far apart are they ? •  How are they clustered ? •  What is the mass of a typical galaxy ? •  What is the mass density of the Universe ?

Page 3: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

Extra-galactic Distances   For extragalactic distances, convenient

unit is 1 Mpc = 106 pc

  Note: Still have m =M at d = 10 pc

m!M = 5 log10 (d / pc)! 5

= 5 log10d

pc"106pc

Mpc

#

$%

&

'(! 5

= 5 log10 (d / Mpc)+ 5log10 (106 )! 5

= 5 log10 (d / Mpc)+ 25

Page 4: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

How many stars in a Galaxy ?   M31 (Andromeda), at 0.9 Mpc, has an

apparent magnitude mV = +3.5 mag   1)   2) Assume M* = +5.5 (Sun-like stars)   3)

  4)

!

M = m " 5 log10(d /Mpc) " 25 = "21.3 mag

FGAL

= n* F*

MGAL

!M* = !2.5 log10FGAL

F*

"

#$

%

&'= !2.5 log10 n*( )

n* =FGAL

F*

=10!(MGAL!M* )/2.5 =10!(!21.3!5.5)/2.5 ( 5)1010

n* = 50 billion stars

Page 5: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

How did Galaxies Form ?

Initial Collapse: Hierarchical Merging: TWO COMPETING SCENARIOS

Elliptical Spiral Irregular

(rotation => slower collapse) (many small high-z galaxies)

(fewer and larger low-z galaxies)

Page 6: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

How did Galaxies Form? Hierarchical Merging •  For:

–  Mergers are seen –  More Ellipticals in high

density clusters –  HST sees more small Irrs

at high z •  Against:

–  Some large Ellipticals seen at high z

–  Irregulars forming today

Initial Collapse •  For:

–  Nearby Ellipticals are old –  Ellipticals seen at high z –  Spirals/Irrs rotating –  Irregulars forming today

•  Against: –  Mergers are seen

PROBABLY BOTH OCCUR

Page 7: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

Galaxy Formation Scenarios

Initial Collapse:

Followed by merging:

Hierarchical merging:

Page 8: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

Colliding Galaxies

Page 9: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

Colliding Galaxies

Page 10: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

The Antennae Galaxy: mid-merger

Page 11: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

Ellipticals Dominate in Clusters

Page 12: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

Cluster Formation Simulation

John Dubinski: www.cita.utoronto.ca/~dubinski “Galactic Canibalism”: forms a giant galaxy at the cluster centre.

Page 13: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

Cluster Formation Simulation

John Dubinski: www.cita.utoronto.ca/~dubinski “Galactic Canibalism”: forms a giant galaxy at the cluster centre.

Page 14: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

How many galaxies are there ?   STEP1: Take all-sky photos

  STEP2: Count galaxies brighter than some magnitude

  STEP3: Assume most galaxies are like the MW*

  STEP4: Calculate depth and volume of sky

  STEP5: Calculate the SPACE DENSITY of galaxies

  [* Big bright galaxies like the Milky Way are easiest to detect.   This does not mean they are the most numerous, just the most visible !]

Page 15: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

Space Density of Galaxies •  Example: The MW has MB = -20 mag. There are ~104 MW-like

galaxies brighter than 14th mag over the whole sky. How many galaxies are there per ( Mpc )3 ?

There is ~1 MW-like galaxy per 100 Mpc3

m!M = 5log10 (d / Mpc)+ 25

d =10(m!M!25)/5=10(14!(!20)!25)/5

= 63 Mpc

Vol =4!

3d

3=

4!

3(63Mpc)3

=106 Mpc3

n =N

Vol=

104gals

106 Mpc3=10!2 gals

Mpc3

Distance modulus equation gives the depth of the survey, i.e. the maximum distance =>

Volume of the survey =>

n = number density

Page 16: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

Typical separation between galaxies: ~(100 Mpc3)1/3 = 4.6 Mpc

However, galaxies are strongly clustered.

How far apart are they ?

Volume: 100 Mpc3 4.6 Mpc

Page 17: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

Large Scale Structure

“The Stickman”: 1980

Geller & Huchra d = v / H0= c z / H0

Galaxy Redshift Surveys

Hubble’s Law used to determine distances

Page 18: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

Large Scale Structure “The Great Wall”: 1988 Galaxy Redshift

Surveys

Page 19: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

Large Scale Structure

CfA redshift survey

Sloan Digital Sky Survey (SDSS)

“Sloan Great Wall”

“Great Wall”

Page 20: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

Large Scale Structure Bubbly Structure: Voids, Walls, Filaments, Clusters.

Page 21: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

Mass-to-Light Ratios •  Assume that a galaxy’s luminosity

is proportional to its mass •  i.e., there is a mass-to-light ratio •  Expressed in solar units:

  X = 1 for our Sun   X ~ 10 for a typical Galaxy

!

M

L= X

M"

L"

Solar Mass

Solar Luminosity

Mass-to-light ratio

Page 22: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

The Mass of Andromeda (M31)   M31 has MV = -21.3 mag. Determine its mass

assuming a “typical” mass-to-light ratio, X = 10.

M =M

LL =10

M!

L!

L =10M!

L

L!

M =10M!10"(MV (M31)"MV

(Sun) )/2.5

M =10# (2#1030 kg)#10"("21.3"5.4)/2.5

!

M = 2 "1041kg =1011M#

Page 23: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

Mass Density of the Universe

•  Multiply ( the space density of galaxies ) x ( the mass of a typical galaxy ) = the mass density of the Universe:

•  This is the luminous matter, i.e. the stars (+gas+dust), that we can see.

•  However … “Dark Matter” dominates. !

" = nM ~1011

M#

100 Mpc3=109 M#

Mpc3$10%28 kg / m3

Page 24: AS1001:Extra-Galactic Astronomystar-kdh1/eg/eg03.pdf · – Irregulars forming today Initial Collapse • For: – Nearby Ellipticals are old – Ellipticals seen at high z – Spirals/Irrs

•  More accurate observations (using masses from the velocities of stars inside galaxies, and of galaxies inside clusters) gives a total density (including both luminous and Dark Matter):

•  Most of matter is “Dark Matter” ! •  Mass of hydrogen atom: mH = 1.7x10-27 kg •  Spread the matter smoothly, and there would be

only a few hydrogen atoms per m3. •  The air we breathe has ~ 1025 atoms per m3.

!

" ~ 3#1010M$

Mpc3~ 3#10%27kg/m3

Mass Density of the Universe