Definitions and Explanations Flashcards

1
Q

galaxies appear to be

A

clustered

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
2
Q

evidence of galaxy clustering

A

projected distribution of galaxies in the sky

redshift surveys.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
3
Q

Redshift survey

A

reveals patterns in the galaxy distribution i.e. clusters, sheets and voids.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
4
Q

peculiar motion

A

is caused by galaxy clusters’ gravitational interaction with the other cluster members.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
5
Q

Superclusters

A

galaxy clusters are themselves clustered and are organised into larger-scale structures

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
6
Q

luminosity indicators

A

RR Lyrae stars and Cepheid variable stars

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
7
Q

Hubble’s constant measures

A

the expansion rate of the Universe

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
8
Q

The standard model for the origin and evolution of the Universe is called

A

the Hot Big Bang model

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
9
Q

Cosmological Principle

A

The universe is homogeneous and isotropic:

universe homogeneous = no matter where you are in it

universe isotropic = no matter what direction you look in

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
10
Q

Galaxies can be thought of as

A

local disturbances in an otherwise perfectly homogeneous and isotropic Universe.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
11
Q

The scale factor measures

A

the characteristic size of the Universe at time t.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
12
Q

the proper distance

A

Is the physical distance between two objects in the Universe.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
13
Q

the co-moving separation

A

is the separation of two objects in a coordinate system that expands along with the expansion of space-time.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
14
Q

a(t) is not a constant in

A

time, but is a constant in space at any given time.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
15
Q

Hubble time, τ

A

sets the timescale for the expansion of the Universe

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
16
Q

Hubble time : t(0) < τ is when

A

including the effects of gravity

gives an age of the universe smaller than the hubble time

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
17
Q

number of things in defence of homogeneity and isotropy

A
  1. The Hubble-Lemaitre Law
  2. The cosmic microwave background radiation
  3. Primordial nucleosynthesis
  4. The age of the universe
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
18
Q

Statement of Olber’s Paradox

A

‘why is the sky dark at night’

if the Universe is infinite in extent and eternal, with stars roughly uniformly distributed throughout space. Every line of sight will intercept a star, so that the whole night sky should be as bright as the surface of a star.

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
19
Q

Resolution of Olber’s Paradox

A
  1. Stars have finite lifetimes
  2. The speed of light is finite
  3. The universe has a finite age.
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
20
Q

Hubble-lemaitre law is a natural consequence of

A

the cosmological principle

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
21
Q

The Friedmann equation describes

A

how gravity acts against the expansion of the Universe

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
22
Q

the constant k defines

A

the geometry or curvature of the Universe, it determines how a(t) evolves with time

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
23
Q

three classes of solutions depending on values of k:

A

k > 0: the universe is closed, with positive curvature

k < 0: the universe is open, with negative curvature

k = 0: the universe is flat, with zero curvature

24
Q

p(c) is

A

the density required to just close the Universe
If p > p(c) the universe recollapses
if p < p(c) the universe expands indefinitely

25
density parameter has three classes of solutions:
Ω > 1 implies Universe is closed Ω < 1 implies Universe is open Ω = 1 implies Universe is flat
26
Although Ω can change with time it can be shown that
its state of being closed, open or flat cannot change
27
the mass continuity equation tells us
that in a steady state, the rate at which mass enters a system is equal to the rate at which mass leaves the system
28
in a matter-dominated universe p ~ in a radiation-dominated universe p ~
p ~ 1/a^3 p ~ 1/a^4
29
the mass continuity equation has three resulting solutions:
k < 0: a(dot) -> c√-k - open universe k > 0: a(dot) = 0 at some critical radius a(c), and a collapse phase starts after a = a(c) - closed universe k = 0: a(dot) -> 0 at t -> ∞ - flat universe
30
temporal behaviour of the scale factor is given by
a(t) ∝ t^2/η a(t) ∝ { t^2/3 matter-dominated { t^1/2 radiation-dominated
31
the effect of the pressure term P is to
slow down the expansion
32
Galaxy rotation curves
the observed rotation velocities are greater than those expected from the gravitational influence of the luminous stars alone, Indicating the presence of a dark matter halo surrounding the galaxy
33
virial theorem assumes
galaxies can be seen as being in a fluid in hydrostatic equilibrium
34
other methods for identifying dark matter
1. gravitational lensing 2. nucleosynthesis 3. studying the pattern of temperature variations in the CMBR
35
for any η of interest Ω ->
1 as z -> ∞ in the Early Universe
36
in the case where Ω(0) < 1
we can expect a fast decrease from Ω = 1 to Ω -> 0. Hence any value of Ω(0) which is not ~1 or ~0 would place us at a very special time.
37
Dark matter candidates
Baryonic: 1. Gas clumps in galaxy halos and clusters 2. MACHOS 3. Low surface brightness galaxies Non-Baryonic: 1. WIMPs 2. Primordial black holes
38
hot dark matter
non-baryonic dark matter was moving relativistically at the time of decoupling from baryonic matter
39
cold dark matter
non-baryonic dark matter was moving non-relativistically at decoupling.
40
Jeans mass
how much mass can you have in a given volume of space before it starts to collapse under its own weight
41
Gravitational collapse will occur when
the characteristic length L of the perturbation is larger than Jean's length λ(J).
42
stable oscillations
If M < M(J) or L < L(J)
43
Jeans instability is not
fast enough to create large-scale structures
44
c^2(s) = γp^(γ-1)
γ is the ratio of specific heats such that γ = 5/3 for adiabatic process and γ = 4/3 for isothermal process
45
Hubble flow
Will produce time-independent coefficients in the density equation The exponential law is replaced by a power law Jeans mass still persists allowing for an expanding universe Fragmentation less plausible as an explanation for the observed mass distribution
46
open universe
universe expands forever
47
closed universe
the universe will stop expanding and will then contract
48
flat universe
the expansion will slow down unit it stops at t -> ∞
49
newtonian cosmology
the study of the evolution of the Universe using only Newton's law to describe gravity
50
matter dominated
corresponds to the epoch where the evolution of the Universe is dominated by 'matter', i.e. non relativistic particles exerting negligible pressure
51
radiated-dominated
corresponds to the epoch where the evolution of the Universe is dominated by relativistic particles exerting a non-negligible pressure
52
graph of how d(diam) varies with redshift z
see notes
53
How the viral theorem can lead to infer the existence of dark matter
Measure o(vr) and the effective radius of the cluster to obtain an estimate of gravitating matter in the cluster On comparison there is a discrepancy between the measurements and theory invokes the existence of dark matter
54
Luminosity distance
The distance to the object implied by the observed flux
55
Angular diameter distance
Is the distance implied by the small angle approximation
56
If γ < 4/3
Jeans mass decreases with increasing density Isothermal collapse
57
If γ = 5/3
An adiabatic process and therefore jeans mass increases with density Gravitational collapse halts.