Gravitation Flashcards

1
Q

What does it mean if a line element is proportional to the minkowski line element?

A

Angles are preserved
*another word for this I can’t remember

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2
Q

How can we show that an object is a tensor?

A

Show that it transforms like a tensor (i.e: with an appropriate jacobian matrix for each index)

*inverse jacobian matrix for lowered indices

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3
Q

How does a metric tensor transform?

What is the definition of the jacobian matrix?

A

Check wall notes (not written out explicitly).
Also make sure to get the definition of the jacobian matrix.

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4
Q

What is the difference between an ordinary derivative and a covariant derivative?

What about an absolute derivative (along a curve)?

A

Mathematical definition is given in the formula sheet.

A covariant derivative tells us about the genuine change in a function over a manifold, including effects from the changing basis vectors with a term in the affine connection.

Absolute derivative parametrises change along a curve - then use chain rule with a covariant derivative.

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5
Q

What does the affine connection describe?

A

Describes how basis vectors vary infinitesimally over the manifold.
*symmetric in bottom two indices
*not a tensor (doesn’t transform like a tensor)

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6
Q

What is the equation of an affinely-parametrised affine geodesic?
How can it be derived?

A

Check wall notes
Derived via transforming N2: a = 0 into curved space from flat space.

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7
Q

How can we find the connection by comparing formulae for affine and metric connections.

A

Apply E-L equations to the effective lagrangian.
L_eff given in Wall notes.
*this gives the minima of the line element between two points: METRIC connection.

Compare this to the equation of an affinely-parametrised affine geodesic to deduce the components of the connection.

*In a tortion-free manifold, metric and affine connections are identical.

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8
Q

How can we lower / raise indices?

A

Apply the metric / inverse metric.

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9
Q

What is the connection for minkowski (flat) space?

A

0

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10
Q

What is the significance of the effective Lagrangian where the geodesic is parametrised by proper time?

A

Constant along the geodesic, equal to either:

+1 : time-like geodesic (trajectory of massive particle)
0 : light-like geodesic (trajectory of light)
-1 : space-like geodesic (unphysical)

L_eff can be shown to be constant by differentiating w.r.t. the geodesic parameter, and applying the equation of an affinely-parametrised affine geodesic.
*also must use the form of the christoffel symbols

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11
Q

What is the Ricci identity?
(What does the Riemann Tensor represent?)

A

The commutator of covariant derivatives acting on a vector is equal to the riemann tensor acting on the vector [check wall notes].

The riemann tensor represents the difference between parallel transporting along different paths to the same destination.

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12
Q

What is the relationship between the Ricci tensor and the Riemann tensor?

What about the Ricci scalar?

A

The Ricci tensor (2-tensor) is the only non-zero contraction of the Riemann tensor (1st and 3rd indices).
In 2D and 3D the Ricci tensor completely describes the Riemann tensor.

The Ricci scalar is the only non-zero contraction of the Ricci tensor (trace). Referred to sometimes as the curvature.
In 2D the Ricci scalar completely describes the Riemann tensor.

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13
Q

What are the symmetries of the Riemann tensor?

A

Considering Riemann tensor with all indices lowered:

Antisymmetric in 1 <=> 2 or 3 <=> 4.
Symmetric in 1,2 <=> 3,4.
Cyclic symmetry in 2,3,4 (sum of all three cycles = 0)

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14
Q

What is the definition of the Einstein tensor and what are its key properties?

A

Check wall notes!
Ricci tensor - 1/2 * metric tensor * Ricci scalar

The Einstein tensor summarises the curvature of a manifold in a covariantly-conserved way. (i.e: covariant derivative of the tensor = 0)

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15
Q

What is a general expression for the stress-energy tensor?
-for a dust
-for a fluid

A

Dust: co-moving energy density / c^2 * two 4-velocities with different indices.

Fluid: Same as dust but density + pressure instead of density. Also extra term: - Pressure * metric tensor

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16
Q

How do we know that the stress-energy tensor is covariantly conserved?

A

Covariant conservation of the stress-energy tensor is equivalent to the continuity equation (energy conservation).

+ energy flux <=> momentum density
momentum density = -d/dx stress tensor

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17
Q

What is Einstein’s equation?
How do we get to the trace-reversed version?

A

Einstein tensor = K * Stress-energy tensor

Contract with inverse metric to get to trace-reversed version.

K = 8 pi G_N / c^4 recovers Newtonian gravity in the non-relativistic limit.

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18
Q

How can we parametrise the weak gravity limit?

A

Metric equal to minkowski metric + h
where h is a metric with determinant much less than 1
( - h for the inverse metric)
Expand in h

The connection can be written simply in terms of h.

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19
Q

What is the source term for gravitational waves?

A

The second time derivative of the moment of inertia (second moment of mass).
*i.e: fast acceleration with large oscillation in quadrupole moment produces large amplitude gravitational waves.

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20
Q

What steps do we take to reach the schwarzschild solution?

A

Use general spherically-symmetric line element.
ds^2 = e^nu dt^2 - e^lambda dr^2 - r^2(dtheta^2 + sin^2(theta)dphi^2)
* nu and lambda dependent on r and t generally.

Find the connection using L_eff.
Construct the Riemann tensor -> Ricci tensor and scalar

Apply the free space Einstein’s equation.
Use gauge freedom to remove final free parameter (change t coordinate).

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21
Q

What is the schwarszchild radius?

A

2GM / c^2

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22
Q

What is Birkhoff’s theorem?

A

Spherically symmetric vacuum solutions can always be made static by a suitable choice of variables.
* so spherically symmetric mass distributions cannot emit gravitational waves.

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23
Q

What are the 4 classical tests of GR in the solar system?

A

Gravitational redshift
Light deflection
Perihelion precession
Light delay

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24
Q

At what rate does an observer at fixed coordinates in a gravitational well measure time passing?
How is this related to the frequency of light they emit/detect?

A

Consider schwarzschild line element for fixed spatial coordinates.
In this case the line element is equal to proper time.

dt / dtau gives the rate at which time is measured to pass. This is directly proportional to the frequency of light that is measured/emitted.

Consider the ratio of these rates for different positions in the well. For a distant observer, consider one of the positions as infinitely far from the source.

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25
Q

Geodesics for schwarzschild solution (given in formula sheet).
-what does l refer to?
-which is the non-classical term?
-which term should be considered the effective potential?

A

l is the angular momentum (per unit mass):
r^2 phi(dot)

The non-classical part is the term in l^2 r_s / r^2

The term in square brackets is the effective potential. The other term on the RHS is a constant - total energy.

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26
Q

What is the requirement for a stable circular orbit?

A

Energy = Potential at that radius.
Potential’ = 0
Potential’’ > 0 (otherwise unstable)

i.e: the bottom of a trough in V_eff

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27
Q

What property do particles coming from infinity have? (orbital dynamics)

A

E > 0

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28
Q

How can we consider the orbital dynamics of a photon?

A

Set K = 0 (null geodesic (light-like))
Set epsilon = 1 {it is really more complicated than this, we must reparametrise as tau is no longer a good choice of coordinate (->inf for massless). This reparametrisation is equivalent to setting epsilon = 1}

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29
Q

What are some interesting properties of the orbital dynamics of a photon?

A

Orbit is independent of photon energy.
V_eff shape is independent of angular momentum, just the normalisation.

30
Q

What does V_eff look like in the schwarzschild solution, for:
-classical?
-massive particles?
-massless particles?

A

Check notes

31
Q

What is perihelion precession?

A

The GR correction to V_eff makes it clear that elliptical orbits do not exist –> they precess.

32
Q

What factors cause light delay?

A

Light delay is the fact that light takes longer to reach us if it passes near a gravitational source, this is due to:
-curved path
-gravitational redshift (usually dominant)

33
Q

What is the impact parameter?
What about for light?

A

The distance between the trajectory (extrapolated from infinity) and the source.

b = l / r{dot} = l / sqrt(2 E_m)

for light b = l (natural units)

*l in this case is angular momentum per unit mass r^2 theta{dot}

34
Q

What is the difference between homogeneity and isotropy?

A

Homogeneous: universe is the same at all distance scales

Isotropic: universe is the same in all directions

35
Q

What is Schur’s theorem?

A

Maximally symmetric spaces (homogeneous+isotropic) are manifolds of constant curvature. This leads to the FLRW metric.

  • This leads to a simplified form of the reimann tensor
36
Q

What is the meaning of “a” in the FLRW metric?
What r coordinate is used in the form of the metric given in the formula sheet?

A

a is the “scalefactor of the universe” = sqrt(current curvature / future curvature)
a = 1 currently

Applying 1/a to distance measure r gives a co-moving coordinate, such that galaxies are not moving away from us in this coordinate.

co-moving coordinate = r/a

37
Q

How does the curvature of the universe evolve over time?

A

Never changes sign
K=0 stays constant but is in unstable equilibrium.

38
Q

What is conformal time?

A

dt = a * d(conformal time)

Using the conformal time gives a FLRW metric that is conformally equivalent to minkowski space given current flat universe.

39
Q

What is the definition of the hubble parameter H?

A

a{dot} / a

40
Q

What is the definition of the deceleration parameter q?

A

-a{doubledot} a / a{dot}^2

positive q means deceleration of the universe

41
Q

What is the current measured value of the hubble constant and the deceleration parameter?

A

H_0 ~ 70 km per s per Megaparsec
q_0 ~ -0.5 : acceleration

42
Q

How do we derive the Friedmann equations?

A

Obtain the Ricci tensor from the FLRW metric.
Assume cosmic matter-energy is a perfect fluid.
-> get a rho, -P, -P, -P form of the stress-energy tensor (in the co-moving frame).

43
Q

What is missing from the Friedmann equations given in the formula sheet?

A

A term -1/3 * the cosmological constant.

44
Q

What is the “third” Friedmann equation?

A

Energy conservation / fluid flow equation
(equivalent to the first law of thermodynamics: expansion <=> work)
Comes from covariant conservation of the stress-energy tensor.

*check wall notes

45
Q

What motivates the treatment of the cosmological constant as dark energy?

A

The cosmological constant terms in the Friedmann equations can be absorbed into energy density and pressure with a mapping.
This mapping leads to the idea of dark energy with equation of state: energy density = -pressure

46
Q

How can we get the equations of state for matter, radiation and dark energy?

A

Use the the fluid flow equation to get an equation in da / drho

Matter: 0 pressure
Radiation: energy density = 3P
Dark energy: energy density = -P

47
Q

What does k_0 refer to in the Friedmann equations?

A

The current curvature of the universe

48
Q

How is the critical density defined?

A

The density which gives a flat universe

= (3 / 8 pi G) * H_0 ^2

49
Q

How can we get an equation to study the evolution of the curvature of the universe?

A

Consider the Friedmann equations where we define Omega = the sum of Omega for matter, radiation, and dark energy

=> Omega - 1 = K_0 / a{dot}^2

50
Q

How do we define Omega when considering the Friedmann equations?

A

The density of some cosmic substance / the critical density.

We can define a similar notion for curvature:
- K_0 / H_0 ^2

51
Q

What issues in cosmology motivate the theory of cosmic inflation?

A

The horizon problem
-we know from the CMB that there are regions of space that should never have been in causal contact and so should not be in thermal equilibrium

The flatness problem
-the current universe is ~ flat, a point of unstable equilibrium. The early universe must have been flat to an extremely precise degree.

52
Q

What is cosmic inflation?

A

A period of vacuum energy dominance in the very early universe leading to extreme growth. This kind of inflation drives curvature to 0 exponentially. Cosmic inflation also solves the horizon problem.

53
Q

What approximation should we make to study the evolution of the universe?

A

As radiation forms a relatively small proportion of the energy in the universe, ignore this contribution.

We can then get equations for the deceleration parameter and the scalefactor of the universe in terms of densities of matter and dark energy.

54
Q

What are the equations governing the fate of the universe?

A

q_0 = 1/2 (Omega_m_0 - 2 Omega_de_0)

Check other one on wall notes

*these can be derived from the friedmann equations by neglecting radiation.

55
Q

What is the weak equivalence principle?

A

A “freely-falling frame” must be indistinguishable from an inertial frame.

56
Q

What is the strong equivalence principle?

A

A rest frame in a gravitational field g is indistinguishable from a frame accelerating with acceleration g. (Locally)

57
Q

What is the relationship between the line element and the metric tensor?

A

Check wall notes

58
Q

What is the definition of the coordinate transformation matrix?

A

Check wall notes

59
Q

How can we use the form of the covariant derivative given in the formula sheet to express the covariant derivative of tensors with raised indices?

A

For each raised indice use a plus instead of minus. Also the indices of the connection will need to be changed.

60
Q

What is the defining equation of an affinely-parametrised affine geodesic?

A

Check wall notes
(tangent vector form as well as connection form)

61
Q

What does rindler space look like?

A

Check notes

62
Q

When we are investigating the dynamics of light rays in schwarzschild space, what should we use as an affine parameter?

A

Use u = epsilon tau

(tau –> 0 as m –> 0)

  • any linear function of an affine parameter is also an affine parameter
63
Q

What does epsilon refer to in the equation for geodesics of the schwarzschild solution?

A

Epsilon is the constant obtained by considering the E-L equations for time given by the schwarzschild metric.

epsilon = (1 - r_s / r) dt/dtau

64
Q

What does t refer to in the FLRW metric?

A

Cosmic time
(time in the cosmic frame - in which the CMB is stationary)

65
Q

What is an isotropic tensor?

A

An isotropic tensor has the same form in all bases.
Scalars are always isotropic.
Vectors are never isotropic.
Rank-2 isotropic tensors = constant * delta
Rank-3 = constant * levi-cevita

66
Q

What does it mean for something to be covariantly conserved?

A

Covariant derivative w.r.t. one of the indices of the object = 0

*equivalent of a vector conservation law

67
Q

What is the covariant derivative of the metric (no common indices)?

A

0

68
Q

What is the inverse metric acting on the metric (1 common index)?

A

Dirac delta

->trace of this gives d, the dimensionality

69
Q

How can we get the Ricci tensor from the form of the Riemann tensor with all indices lowered?

A

Apply the metric appropriately
The same should be done to find the Ricci scalar.

70
Q

What does w refer to?

A

The equation of state P / rho