Astr 5460 Wed., Nov. 3, 2004
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This week: Large Scale Structure |
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(Ch. 11, Combes et al., parts) |
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Unless noted, all figs from Combes et al. |
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Already talked about galaxy clusters a
lot, and some distance ladder topics will be covered in more detail in Mike
Pierce’s class next semester. |
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Some other issues
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Discuss homework |
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Not as great as expected – just busier
now? Can turn in problem 6 next week
for extra credit – please write up the process! |
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Discuss Observing Project (briefly!) |
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Mid-term exam: |
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2 hours, take-home, on your honor, only
calculator and constants/conversions |
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Some “basic knowledge” questions in
addition to more analytic problems.
Know terms, definitions, other intangible issues. |
Large Scale Structure
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Galaxy structure – how is the mass in
the universe distributed (and recall gas can be important, too!)? Homogeneous? On what scale? |
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Text is a bit old (fine for history),
but the best newest information will come from SDSS and 2dF. CHECK IT OUT! |
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Background radiation also of interest
(discrete sources vs. true diffuse background). |
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Background “SED”
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CMBR of special interest (as we will
get to) and X-ray is a recent development (CXO). |
Distance Scales
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Parallax and Trigonometric Methods: |
Distance Scales
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Parallax and Trigonometric Methods |
Distance Scales
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Parallax and Trigonometric Methods |
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tan λ = Vt/Vr = μd/Vr |
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So then d = Vr tanλ/4.74μ
[pc] |
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Where velocities are in km/s and proper
motion μ is in arcseconds per year. |
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Should be something you can derive (it
would be a good problem to work in your free time) |
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Distance Scales
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Parallax and Trigonometric Methods –
once Hyades distance known, can use main-sequence cluster fitting. |
Distance Scales
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Parallax and Trigonometric Methods –
once Hyades distance known, can use main-sequence cluster fitting. |
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Then employ the distance modulus,
basically a vertical shift on the CMD diagram, (m-M = 5 logd(pc) -5) |
Distance Scales
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Cepheids and Standard Candles |
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Various stars in the instability strip
of the H-R diagram with Period-luminosity relations. |
Distance Scales
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Cepheids and Standard Candles |
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Various stars in the instability strip
of the H-R diagram with Period-luminosity relations. |
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Figures for Cepheids from Horizons
(Michael Seeds) |
Distance Scales
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The Tully-Fischer Relation |
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L = kΔVα – where
the index is ~ 4. |
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Better in the near-IR, as we discussed
before, less star formation visible at H-band, so less distortion. |
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The velocity dispersion comes from
either 21 cm or stellar optical absorption lines. |
Distance Scales
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This is where Combes et al. discusses
the Hubble Law: |
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Vr = Hod where Ho is in
km/s/Mpc |
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Hubble constant Ho is independent of
direction in the sky (that’s important, think about it!) |
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Also recall Ho = h 100 km/s/Mpc |
Distance Scales
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The Tully-Fischer Relation |
Distance Scales
Distance Scales
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The Sunyaev-Zeldovich Effect: |
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Look toward hot intercluster medium in
galaxy clusters…Thomson scattering can affect the CMBR seen through such a
medium |
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Optical thickness is τT
= ∫σTne dl |
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Cluster properties can indeed “hamper”
the CMBR |
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The CMBR is heated by the ICM, altering
the frequency: Δν/ν = 4kTe/mec2,
leading to: |
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ΔT/T = - ∫ 2kTe/mec2
dτT (hν << kTe) |
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At low frequencies, REDUCES the
temperature of the CMBR. |
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Can get distance estimates from S-Z
effect. |
Distance Scales
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The Sunyaev-Zeldovich Effect |
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Measure the X-ray flux, the temperature
fluctuations, and the temperature, and can get distance, and hence Ho. |
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Compton effect here |
Distance Scales
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Surface-Brightness Fluctuations |
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Surface brightness does not vary with
distance – why? |
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How about, say, the number of stars per
pixel as a function of distance? That
does change, and the statistical uncertainty does vary with distance. |
Distance Scales
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Surface-Brightness Fluctuations |
The “Third Dimension”
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Galaxy distributions seen in images are
2-d projections on the sky. |
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Need distances…easiest way is to use
the Hubble flow and redshifts, either photometric or spectra (best). |
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Reminder – SDSS and 2dF rule here now. |
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Huchra and Gellar’s “Z-machine” for the
CfA survey as recounted in “Lonely Hearts of the Cosmos” by Dennis Overbye –
Great! |
The “Third Dimension”
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Look at distance “slices” here. |
The “Third Dimension”
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The famous “man” in the
distribution. Shows walls, voids, etc. |
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Why elongations, “finger of god”
distributions pointing at “us?” |
Statistical Methods
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Correlation functions |
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How do you measure, quantitatively, the
tendency of galaxies to cluster? |
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Following is specifically from Longair,
but also present in Combes et al. with a different presentation. |
Large-scale Distribution
of Galaxies
Large-scale Distribution
of Galaxies
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On small scales, the universe is very
inhomogeneous (stars, galaxies). What
about larger scales? |
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Angular two-point correlation function
w(θ): |
Large-scale Distribution
of Galaxies
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This function w(θ) describes
apparent clustering on the sky down to some magnitude limit. |
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More physically meaningful is the
spatial two-point correlation function ξ(r) which describes clustering
in 3-D about a galaxy: |
Large-scale Distribution
of Galaxies
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w(θ) isn’t so hard to measure from
various surveys – just need positions. |
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ξ(r)
is harder – must have redshifts to do properly. Can make some assumptions however. |
Large-scale Distribution
of Galaxies
Large-scale Distribution
of Galaxies
Large-scale Distribution
of Galaxies
Large-scale Distribution
of Galaxies
Large-scale Distribution
of Galaxies
Large-scale Distribution
of Galaxies
Large Scale Motions
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Milky Way motion vs. CMBR, a “dipole”
with velocity of about 1000 km/s (from COBE) |
Large Scale Motions