lecture 21 cosmological models

39
Lecture 21 Cosmological Models ASTR 340 Fall 2006 Dennis Papadopoulos

Upload: aurora

Post on 24-Feb-2016

64 views

Category:

Documents


0 download

DESCRIPTION

Lecture 21 Cosmological Models. ASTR 340 Fall 2006 Dennis Papadopoulos. Spectral Lines - Doppler. Doppler Examples. Doppler Examples. = R now /R then. Expansion Redshifts. z=2 three times, z=10, eleven times. Expansion Redshifts. Expansion - Example. Current Record Redshift. - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: Lecture 21 Cosmological Models

Lecture 21Cosmological Models

ASTR 340Fall 2006

Dennis Papadopoulos

Page 2: Lecture 21 Cosmological Models

Spectral Lines - Doppler

Page 3: Lecture 21 Cosmological Models

obs em

em

z

1 em

obs

z

Page 4: Lecture 21 Cosmological Models

Doppler Examples

Page 5: Lecture 21 Cosmological Models

Doppler Examples

Page 6: Lecture 21 Cosmological Models

Expansion Redshifts

= Rnow/Rthen

z=2 three times, z=10, eleven times

Page 7: Lecture 21 Cosmological Models

Expansion Redshifts

Page 8: Lecture 21 Cosmological Models

Expansion - Example

Page 9: Lecture 21 Cosmological Models

Current Record Redshift

Page 10: Lecture 21 Cosmological Models

Hubbleology

• Hubble length DH=c/H ,• Hubble sphere: Volume enclosed in Hubble

sphere estimates the volume of the Universe that can be in our light-cone; it is the limit of the observable Universe. Everything that could have affected us

• Every point has its own Hubble sphere• Look-back time: Time required for light to travel

from emission to observation

Page 11: Lecture 21 Cosmological Models

Gravitational Redshift

Page 12: Lecture 21 Cosmological Models

Interpretation of Hubble law in terms of relativity

• New way to look at redshifts observed by Hubble • Redshift is not due to velocity of galaxies

– Galaxies are (approximately) stationary in space… – Galaxies get further apart because the space between

them is physically expanding!– The expansion of space, as R(t) in the metric equation, also

affects the wavelength of light… as space expands, the wavelength expands and so there is a redshift.

• So, cosmological redshift is due to cosmological expansion of wavelength of light, not the regular Doppler shift from local motions.

Page 13: Lecture 21 Cosmological Models

Relation between z and R(t)• Using our relativistic interpretation of

cosmic redshifts, we write

• Redshift of a galaxy is defined by

• So, we have…

em

emobsz

obs RpresentRemitted

em

zRpresentRemitted

1Rpresent Remitted

Remitted

RR

Page 14: Lecture 21 Cosmological Models

Hubble Law for “nearby” (z<0.1) objects

• Thus

where Hubble’s constant is defined by

• But also, for comoving coordinates of two galaxies differing by space-time interval

d=R(t)Dcomoving , have v= Dcomoving R/t=(d/R)(R/t)• Hence v= d H for two galaxies with fixed

comoving separation

H 1R

Rt

1RdRdt

cz cRR

ct(R /t)R

dlight travel H

Page 15: Lecture 21 Cosmological Models

Peculiar velocities• Of course, galaxies are not precisely at fixed

comoving locations in space• They have local random motions, called

“peculiar velocities”– e.g. motions of galaxies in “local group”

• This is the reason that observational Hubble law is not exact straight line but has scatter

• Since random velocities do not overall increase with comoving separation, but cosmological redshift does, it is necessary to measure fairly distant galaxies to determine the Hubble constant accurately

Page 16: Lecture 21 Cosmological Models

Distance determinations further away

• In modern times, Cepheids in the Virgo galaxy cluster have been measured with Hubble Space Telescope (16 Mpc away…)

Virgo cluster

Page 17: Lecture 21 Cosmological Models

Tully-Fisher relation• Tully-Fisher relationship (spiral galaxies)

– Correlation between • width of particular emission line of hydrogen,• Intrinsic luminosity of galaxy

– So, you can measure distance by…• Measuring width of line in spectrum• Using TF relationship to work out intrinsic luminosity of galaxy• Compare with observed brightness to determine distance

– Works out to about 200Mpc (then hydrogen line becomes too hard to measure)

Page 18: Lecture 21 Cosmological Models

Hubble time• Once the Hubble parameter has been determined accurately, it

gives very useful information about age and size of the expanding Universe…

• Recall Hubble parameter is ratio of rate of change of size of Universe to size of Universe:

• If Universe were expanding at a constant rate, we would have R/t=constant and R(t) =t(R/t) ; then would have H= (R/t)/R=1/t

• ie tH=1/H would be age of Universe since Big Bang

H 1R

Rt

1RdRdt

R(t)

t

Page 19: Lecture 21 Cosmological Models

Modeling the Universe

Chapter 11

Page 20: Lecture 21 Cosmological Models

BASIC COSMOLOGICAL ASSUMPTIONS

• Germany 1915:– Einstein just completed theory of GR– Explains anomalous orbit of Mercury perfectly– Schwarzschild is working on black holes etc.– Einstein turns his attention to modeling the

universe as a whole…• How to proceed… it’s a horribly complex

problem

Page 21: Lecture 21 Cosmological Models

How to make progress…• Proceed by ignoring details…

– Imagine that all matter in universe is “smoothed” out– i.e., ignore details like stars and galaxies, but deal

with a smooth distribution of matter• Then make the following assumptions

– Universe is homogeneous – every place in the universe has the same conditions as every other place, on average.

– Universe is isotropic – there is no preferred direction in the universe, on average.

Page 22: Lecture 21 Cosmological Models

• There is clearly large-scale structure– Filaments, clumps– Voids and bubbles

• But, homogeneous on very large-scales.• So, we have the…• The Generalized Copernican Principle… there

are no special points in space within the Universe. The Universe has no center!

• These ideas are collectively called the Cosmological Principles.

Page 23: Lecture 21 Cosmological Models

Key Assumptions

Page 24: Lecture 21 Cosmological Models

Riddles of Conventional Thinking

Page 25: Lecture 21 Cosmological Models

Stability

Page 26: Lecture 21 Cosmological Models

GR vs. Newtonian

Page 27: Lecture 21 Cosmological Models

Newtonian Universe

Page 28: Lecture 21 Cosmological Models
Page 29: Lecture 21 Cosmological Models

Expanding Sphere

Page 30: Lecture 21 Cosmological Models

Fates of Expanding Universe

Page 31: Lecture 21 Cosmological Models

Spherical Universe

Page 32: Lecture 21 Cosmological Models

Friedman Universes

Page 33: Lecture 21 Cosmological Models

Einstein’s Greatest Blunder

Page 34: Lecture 21 Cosmological Models
Page 35: Lecture 21 Cosmological Models

THE DYNAMICS OF THE UNIVERSE – EINSTEIN’S MODEL

• Einstein’s equations of GR

TG 4

8cG

“G” describes the space-time curvature (including its dependence with time) of Universe… here’s where we plug in the RW geometries.

“T” describes the matter content of the Universe. Here’s where we tell the equations that the Universe is homogeneous and isotropic.

Page 36: Lecture 21 Cosmological Models

• Einstein plugged the three homogeneous/isotropic cases of the FRW metric formula into his equations of GR to see what would happen…

• Einstein found…– That, for a static universe (R(t)=constant), only the spherical

case worked as a solution to his equations– If the sphere started off static, it would rapidly start collapsing

(since gravity attracts)– The only way to prevent collapse was for the universe to start off

expanding… there would then be a phase of expansion followed by a phase of collapse

Page 37: Lecture 21 Cosmological Models

• So… Einstein could have used this to predict that the universe must be either expanding or contracting!

• … but this was before Hubble discovered expanding universe (more soon!)– everybody thought that universe was static (neither expanding nor contracting).

• So instead, Einstein modified his GR equations!– Essentially added a repulsive component of gravity– New term called “Cosmological Constant”– Could make his spherical universe remain static– BUT, it was unstable… a fine balance of opposing

forces. Slightest push could make it expand violently or collapse horribly.

Page 38: Lecture 21 Cosmological Models

• Soon after, Hubble discovered that the universe was expanding!

• Einstein called the Cosmological Constant “Greatest Blunder of My Life!

• ….but very recent work suggests that he may have been right (more later!)

Page 39: Lecture 21 Cosmological Models

Sum up Newtonian Universe