T1: 2. Manifolds and Tensors Flashcards

1
Q

What does it mean for spacetime to be ‘locally flat’?

A

Around every point, there is a coordinate system which maps a local neighbourhood to a point in the real plane.

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2
Q

Define a coordinate system (and hence, coordinates)

A

A map from a part of spacetime to an open region in the n-dimensional real plane. Coordinates are the collection of corresponding functions.

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3
Q

Define a coordinate transformation

A

The map between two overlapping coordinate systems across the n-dimensional real plane.

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4
Q

Define a chart (coordinate system) in the context of manifolds.

A

Given a set M, a chart is a function phi which forms a bijection between U (the subset of M) and the open subset of the n-dimensional real plane defined by the action of phi on an element of U.

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5
Q

Define an atlas

A

A collection of charts {(U_a, phi_a)}, such that:
- The union of all subsets U = M (i.e. the subsets cover the entire original set).
- If the intersection of a pair of subsets U_a and U_b is not the empty set, the successive map of the inverse phi_b and phi_a is differentiable where it is defined.

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6
Q

Define a maximal altas

A

The collection of all charts which satisfy the atlas conditions.

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7
Q

Define the n-dimensional manifold

A

The pair of a set M and a maximal atlas.

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8
Q

Define the three primary kinds of vectors and which is most suitable on a manifold

A

a. Displacement vector
b. Tangent vector
c. Normal vector

b - Manifolds consider locally flat regions and the tangent vector in infinitesimally small.

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9
Q

Why are displacement vectors not appropriate for use on a manifold.

A

They don’t form a vector space on a manifold: ‘tip to tail’ vector addition is not commutative.

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10
Q

How do we define d/dλ in flat space?

A

V^μ ∂_μ = (dx^μ/dλ) ∂/∂X^μ

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11
Q

Define a tangent vector field

A

A choice of vector V in the tangent vector space at each point p in M; a vector-valued function on M

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12
Q

Define tangent vector space T_p

A

The space of vectors V=d/dλ tangent to M at point p.

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13
Q

Define cotangent space T_p^*

A

The space of linear maps ω from the tangent space to the reals.

I.e. The space of vectors cotangent to M at point p.

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14
Q

How do we define the cotangent vector?

A

A differential function df maps from tangent space to real numbers. We can equate this to the action of the tangent vector on some function f:

df(V) = V(f)

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15
Q

Define cotangent vector field

A

A choice of cotangent vector ω∈ T_p^* at each point p in M.

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16
Q

What is the basis of tangent vectors?

A

∂/∂X^μ

17
Q

What is the basis for covectors?

A

dx^μ

18
Q

How do we coordinate transform components of tangent vectors?

A

By chain rule on the coordinates in the component.

V ̃^μ = V^ν (tilde on top)

Refer to notes

19
Q

How do we coordinate transform components of covectors?

A

By chain rule on the coordinates in the basis vector.

ω ̃_μ = ω_ν (tilde on bottom)

Refer to notes

20
Q

Define a tensor of type [r,s] at a point p.

A

An object which linearly maps r covectors and s vectors to the reals.

21
Q

Define a type [r,s] tensor field

A

An object which gives an [r,s] tensor at each point p on M.

22
Q

What type of tensor is a function?

A

Type [0,0]: scalar

23
Q

What type of tensor is a vector (covector)?

A

Type [1,0] (type [0,1])

24
Q

What type of tensor is Kroneker delta? What is special about it?

A

Type [1,1] with same components in any coordiante system: diag(1, … ,1).

25
Q

What are the three tensor equation rules?

A
  • Free/dummy indices
  • Renaming indices
  • Rearrange kernel symbols as desired
26
Q

Why is a [1,0] tensor a vector?

A

r denotes the number of covectors the tensor takes as an argument and maps to the reals.

This tensor takes one covector and maps it to the reals; the action of a vector.