Astro 1 - Lecture 33


Matthew A. Bershady

Department of Astronomy & Astrophysics

Penn State University


Fall 1996

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© 1995 Matthew A. Bershady

Lectures Lecture page Astro1 page



HUBBLE'S BUBBLE AND COSMIC SPIKES



Questions you should have explored:

Does the large scale structure of galaxy clustering continue
(in space, in size)?

And if so, to what scales? (sizes, distances, masses)

How do we measure this structure?

In other words, how do we measure distances?




1. Revisit the distance ladder


(i) After parallax . . .
. . . all methods of determining distances involve ``standard candles''

(ii) Distances are then estimated via measuring apparent brightness and inferring luminosity

(distance is inferred via the inverse-square law)


So what makes an ideal ``standard candle?''

(a) should be ``standard,'' i.e. well-defined luminosity

(b) should be bright (see it to large distances)


Cepheids are ok, Super Novae are very good, but ...

galaxies are even brighter, and ...

it turns out that the rotation speed and the luminosity of a galaxy are well correlated.

Why?
Both are measures of mass

The Tully-Fisher relation




2. Universal Expansion and Hubble's Law


On average, galaxies are all moving away from each other.

The Universe is expanding

The farther away galaxies are the faster they move away from each other
(to be demonstrated).

The Hubble flow

Recession speed is measured as a Doppler shift of a known spectral feature:

The cosmological redshift:

z = recession speed (v) / c

Hubble diagrams :

recession speed vs. distance

Crucial: Distance must be inferred from some standard candle!

Slope of the relation in the Hubble diagram gives Hubble's constant :

H = 75 km/s / Mpc

Another ``distance indicator:''

Measure recession speed, infer a distance (d):

d = v / H

Assumptions : Expansion and the Universe are

- smooth,

- uniform,

- and appear the same to every observer.




3. Large Scale Structure Revisited


Wide-angle surveys: shallow but broad

vs.

``pencil-beam'' surveys: narrow but deep


Observed: lack of homogeneity in the galaxy distribution

Homogeneous means: the same everywhere

Non-isotropic ?

Isotropic means: looks the same in every direction

Do observations `fly in the face' of Universal Expansion?


The Universe on very large scales is:

neither smooth nor uniform

- large voids (40-100 Mpc)

- clusters and super-clusters (1-40 Mpc)

- The Great Wall

- Structures up to 200 Mpc across!


Compare to total size of observable universe: 4000 Mpc

Large scale structures on scales 5% of this size!


Perhaps only on the largest scales, the Universe looks the same in every direction.




Q33.1 What aspect of the ``Hubble flow'' of galaxies makes it possible to use their velocities to estimate distances?

(a) All galaxies are moving with our galaxy through the Universe.

(b) All galaxies are moving at the same speed.

(c) The speed of light is finite.

(d) The Hubble diagram relates rotation speed to luminosity.

(e) On average, all galaxies move away from each other.


Q33.2 Why do very large scale structures call into question the reality of a uniform expansion?

(a) The ``Hubble flow'' is observed only for small scale structures.

(b) The Universe can't expand if structures are too large.

(c) Large scale structures imply large scale inhomogeneities.

(d) Large scale structures call into question the reality of any expansion.

(e) Uniformity can't occur if there is expansion.


Lectures Lecture page Astro1 page

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Last updated: Nov 5, 1996 Matthew A. Bershady