Lecture 2: Acceleration & Cos Constant Flashcards

1
Q

how to obtain acceleration equation?

A

differentiate the Friedmann equation wrt time

(then sub in fluid equation and simplify)

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2
Q

the acceleration equation (and hence acceleration) is independent of

A

curvature

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3
Q

from the acceleration equation why is the expansion of the universe decelerating

A

if we have normal matter with p>0 and pressure >or=0
then acceleration equation is overall negative

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4
Q

einstein related mass density and energy density via

A

ε=pc^2
making a direct connection between mass and energy

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5
Q

using natural units with c=1 would cause

A

dimensions of k to be [T^-2]

length and time interchangeable

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6
Q

The notion of curvature of space-time demands that we introduce

A

a new metric, capturing the structure of the universe and, therefore, to be used
to define time, distance, curvature and so on.

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7
Q

In 4-dimensional space-time we generalise the notation of co-ordinates as

A

dx^u or dx^v with u and v being indices defining the dimension of space-time to be considered

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8
Q

dx^0

A

dt
time

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9
Q

dx^1

A

dx
x-dimension

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10
Q

dx^2

A

dy
y-dimension

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11
Q

dx^3

A

dz
z-dimension

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12
Q

space time interval between two points

A

use the einstein summation convention
sum of guv dx^u dx^v

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13
Q

einstein summation convention permits us to

A

drop the summation symbol and sum over repeated indices u,v=0,1,2,3

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14
Q

guv

A

metric tensor

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15
Q

robertson-walker metric

A

the most general of homogeneous and
isotropic metrics that also allows for curved space-time

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16
Q

radial geodesic

A

The shortest distance between two points in curved space is then given
by the line dθ = 0, dφ = 0:

17
Q

Observations show that the expansion of the universe is

A

accelerating

18
Q

what does the universe accelerating tell us mathematically

A

expect an extra term in the Friedmann equation - cosmological constant

19
Q

an accelerating universe requires

20
Q

a positive cosmological constant gives

A

a positive contribution to acceleration, acting as
a repulsive force (compared to the force of gravity).

21
Q

if Λ is sufficiently large, it can

A

overcome gravitational attraction, leading to an accelerating universe (with cosmological acceleration) having already been measured.

22
Q

can define an equivalent dimensionless density parameter for Λ which varies with

A

time even though Λ is fixed due to the existence of H in the denominator

23
Q

how are density, geometry and cosmological constant interconnected

A

Ωm+ΩΛ +Ωk=1