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- Today: Classification
and Morphology
- (following ch. 1 of the textbook)
- Unless noted, all figs and
equations from Combes et al. or Longair.
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2
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- Observational Basics – more to come
- Classifications
- Luminosity Distributions
- Stellar Populations, Color
- Some Statistical Properties
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3
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- Initially just a type of nebula
- Hubble resolved stars in M31 (1920s)
- Many mixed catalogs already existed
- Messier (M – “fuzzy non-comets”), 39 of 109
- New General Catalog (NGC), 3200 of 7840
- Today there are many surveys/catalogs (see NED entries while doing
homework)
- SDSS and 2dF (more later this semester)
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4
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5
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- The nuclear bulge is population II
(old stars)
- So the Sa – Sc sequence is consistent with
little gas Þ more gas
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6
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7
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- M87 is a cD galaxy, technically.
Kormendy (1982) distinguishes these from being merely giant
ellipticals.
- Extensive stellar envelope up to 100 kpc
- Only in regions of enhanced galaxy density (a factor of 100 denser than
the average)
- Multiple nuclei in 25-50% of cDs (a very rare thing)
- Regular cD clusters are systems that have relaxed into dynamical
equilibrium.
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8
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- Galaxies live in clusters
- Rich clusters: thousands of
galaxies
- Poor clusters: Fewer than a
thousand
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9
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10
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11
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12
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13
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14
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15
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16
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17
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- Elliptical galaxies have an apparently simple structure, can be
characterized by their luminosity distribution. Maximum in center, and falls off:
- Hubble’s Law:
- De Vaucouleur’s r1/4 Law:
- Log (I/Ie) = -3.33[(r/re)1/4 –
1]
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18
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19
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20
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21
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22
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23
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24
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25
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26
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27
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- The frequency with which galaxies of a particular luminosity are found
in space. Note that
luminosities can be expressed in magnitudes:
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28
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29
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30
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- Solid line is the best fit SCHECHTER (1976) function:
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31
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- Exact parameters depend on sample.
SDSS and 2dF provide the best estimates. Typically slopes around
a = -1, MB = -20 (note for reference that quasars by
definition more luminous than -23).
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32
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- Features to note
- Morphology matters, also field vs. cluster.
- L* or M* in rich clusters isn’t a bad “standard
candle”
- cD galaxies in cluster centers are special cases; they are like massive
ellipticals but have extra stellar envelopes. They do not fit extrapolations
of ellipitical LFs.
- Low luminosity end of LFs not well determined (Irr and dwarf
ellipticals). Again SDSS
will probably be the best word on this (if it goes faint enough).
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33
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34
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35
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36
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37
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38
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- Roberts & Haynes 1994:
- Masses from S0 to Scd roughly constant, then decrease, and M/L roughly
the same – more next chapter
- H I not significant in ellipticals (< 1 in 10000), but is in spirals
(0.01 to 0.15 from Sa to Sm)
- Total surface density decreases, H I surface density increases
- Ellipticals are red, spirals are blue…
- H II regions frequency increases monotonically along the sequence
(Kennicutt et al. 1989)
- Star formation rates appear key to these relations
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39
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- From Hopkins et al. (2001)
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