T2: 1. Geometric Preliminaries and 2. Gravity from Curvature Flashcards

1
Q

What do round brackets in a lower index indicate?

A

Symmetrisation of indices: sum of terms with indexes swapped.

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

What do square brackets in a lower index indicate?

A

Anti-symmetrisation of indices: difference of terms with indexes swapped.

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

What conditions does the weak field limit impose on our model?

A

The metric differs from flat by small addition g_µν = η_µν + h_µν, where h_µν is small.

Objects move slowly: dx^i/ds «

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

What does static mean for the metric in weak field?

A

Its time-independent; ∂_t g_µν= 0.

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

State the perfect fluid stress tensor T^µν

A

T^µν = (ρ + p)U^µU^ν + pg^µν

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

State the Einstein-Hilbert action

A

S[g] = 1/16πG int(d^4x √−g R)

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

How do we add mass to the EH action?

A

We require it to be stationary on the EH action so we define G_µν = 8πGT_µν with T_µν = −2/√−g δS_m[g]/δ_gµν(x)

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

How do we add an EM field to the EH action?

A

Define some field strength tensor with potential Aµ(x):
F_µν(x) = ∇_µA_ν − ∇_νA_µ

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

What is special about the field strength tensor?

A

We can replace the covariant derivatives with partials; the Christoffels from each cancel.

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

How do we vary the inverse metric?

A

δM^-1 = -M^-1 δM M^-1

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