Cosmology: Lets Take A Step Back Flashcards

1
Q

Evidence for the Big Bang

A

Sky is dark at night
CMB
More distant galaxies appear redder

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2
Q

Sky is dark at night

A

If the universe was static and infinite, everywhere was as bright as the sun
So the universe must’ve had a beginning and be dynamic

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3
Q

More distant galaxies appear redder

A

Suggests galaxies are flying away from us
Hubble’s law came from this (old and new)
Really space itself is expanding, prediction of GR
Galaxies don’t really move much
Beginning of universe was dense

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4
Q

CMB

A

All of space has been uniformly filled with matter/radiation
Since early universe there’s been much clumping but it’s still uniform
Beginning of universe was hot

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5
Q

What are the possible geometries of space?

A

Open (saddle)
Closed (sphere)
Flat

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6
Q

What geometry are we in?

A

Flat

Or like a super super flat like patch of smth else

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7
Q

Inflation

A

Extremely extreme physics
The univer goes from less than an atom to like a basket ball in hardly any time at all
Solves problems though

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8
Q

What problems does inflation solve

A

No longer matters what geometry space is
Uniform temp - everything could’ve cooled to equilibrium before inflation
Quantum fluctuations become normal fluctuations become us

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9
Q

Why matter over antimatter (???)

A

Quantum - spontaneous creation (smth from nothing briefly)
Negative gravity energy + positive matter energy = 0?
NEED QUANTUM GRAVITY!

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10
Q

Hubble’s law

A

1) v = Hod
2) d(t) = a(t)do
3) H(t) = v/d
4) a(t) = e^Ht+C
5) e^C = a0 = 1

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11
Q

How to find to

A

To = d/v = d/Hod = 1/Ho

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12
Q

Expansion of universe

A

1) T1 less T0, d1 > d0
2) dE = -PdV
3) P = u/3, u = sigma(T^4)
4) dE = -PdV, d(uV) = -udV/3
5) equate dE = d(uV)
6) product rule
7) V = d^3, get in terms of dV/V
8) u - get in terms of du/u
9) equate them

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13
Q

Newtonian Friedman equation

A

1) E = PE + KE
2) solve for v^2
3) M = density(V)
4) find v^2/r^2
5) v=Hr, r=ar0, H=da/a
6) U = 0, find ro(0)
7) sub back in

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14
Q

Cosmic acceleration

A

1) a = second r derivative (Newtonian)
2) m = Dv
3) v = d/dt(Hr) = d/dt (da/a x ar0)
4) d2r/r = -4piGp/3
5) p = p+3P/c^2

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15
Q

Dark energy - P = -density c^2

A

1) epsilon = roc^2
2) E = epsilonV, E’ = epsilon (V + dV)
3) dE = -W = -PdV
4) dE = E’ - E

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16
Q

Dark energy - a(t) = ?

A

1) P + roc^2 = 0
2) da/a = -4piG/3(Ro + 3P/c^2)
3) matter and dark energy terms, matter is negligible
4) in terms of epsilon
5) plug back in for ro

17
Q

Hubble’s law - 3 scenarios for t0

A

t0 < 1/H0 - expansion slowing down
t0 = 1/H0 - constant expansion
t0 > 1/H0 - accelerating expansion

18
Q

How was the CMB creates

A

Early universe was a hot plasma in thermal equilibrium - Compton scattering so it was opaque
As space expanded, KE of particles lowered so can’t ionize H atoms - universe became transparent

19
Q

Newtonian Friedman equation - 3 cases for da

A

da > 0 - universe expanding
da < 0 - universe contracting
da = 0 - universe is static

20
Q

What does the Friedman equation do?

A

Relates expansion of universe to matter density and shape of space

21
Q

U < 0

A

ro > roc
Big Crunch
Closed positive curvature
Sphere

22
Q

U > 0

A
ro < roc
Matter not dense enough to stop expansion
Big freeze
Infinite, negative curvature, open
Saddle
23
Q

U = 0

A

ro = roc
Matter dense enough to stop expansion but only when universe is infinite
Infinite, open, zero curvature, like flat plane
Total E = 0 - nothing from nothing

24
Q

What do measurements of matter and measurements of CMB suggest?

A

Matter - big freeze (even with dark matter)

CMB - flat (smth is stopping expansion)

25
Q

How does energy density of dark energy change with expansion of space?

A

It’s constant

26
Q

Is negative pressure weird?

A

No, it’s just matter under tension (stretching a balloon)