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PHY 4460 RELATIVITY

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Tell curvature form distances. Write down metric in examples. General line element ... Curvilinear coordinates. Example. Example. Example. Example. Embedding General ... – PowerPoint PPT presentation

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Title: PHY 4460 RELATIVITY


1
PHY 4460RELATIVITY
  • K Young, Physics Department, CUHK
  • ?The Chinese University of Hong Kong

2
CHAPTER 10MATH OF CURVED SPACE THE METRIC
3
Overview
  • Distance and metric
  • chapter 10 (this one)
  • Vectors
  • chapter 12
  • Differentiation
  • chapter 13
  • Curvature
  • chapter 16

4
Objectives
  • Tell curvature form distances
  • Write down metric in examples
  • General line element
  • Embedding (can be omitted)
  • sphere
  • general

5
Objectives
  • Homogeneous manifolds
  • closed, flat, open
  • Schwarzschild
  • Weak field

6
Introduction
  • Gravity spacetime curvature
  • How do we describe curvature

7
Extrinsic
  • We can see that the 2D surface of the earth is
    curved
  • By going out of it to 3D and looking down

8
Extrinsic
  • We can discuss an N dimensional object (e.g. N
    2)
  • By embedding it in a larger M dimensional flat
    object, M gt N (e.g. M 3)
  • And discussing the curvature in M dimensions

Embedding
9
Extrinsic
  • In relativity N 4 (ie. 31)
  • The extra M ? N dimensions are fictitious
  • Make sure physics is independent of these
    fictitious dimensions

10
Intrinsic
  • Can we tell surface of earth is curved
  • While staying on the surface?

11
Intrinsic
  • Can we tell curvature intrinsically?
  • By measuring distances
  • Reduce to infinitesimal distances
  • Assume quadratic form
  • Riemannian geometries
  • All these can be discussed more physically (but
    less rigorously) by embedding

12
Embedding vs Intrinsic
13
Terminology
  • Euclidean / Minkowski

14
Terminology
  • Manifold
  • Manifold ? "space" Not to be confused with
    space in spacetime

15
Coordinates xm
  • Need not all have same units

Grid
  • Not a vector
  • Upper indices
  • Lower indices xm do not exist
  • xm (3, 9)

16
  • Many coordinate systems possible
  • Independence of coordinates

17
  • Coordinate grid
  • Coordinate ? distance
  • e.g. polar coordinate Df ? distance
  • later Dt ? time

18
Central question
  • How is distance Ds
  • related to the change in coordinates Dxm ?

19
Examples ofCoordinates and Distances
20
Examples
  • A flat space x, y
  • B flat space r, f
  • C sphere q, f
  • D sphere r, f
  • E tilted axes

21
A (x, y)
Ds2 Dx2 Dy2
22
Ds2 Dx2 Dy2 Ds2 is a linear function of the
quadratics Dx2, Dy2
23
B (r, f)
x r cosf y r sinf
Ds2 Dr2 r2Df 2
24
DeriveD s2 D r2 r2Df 2
25
Method 1
Ds2 Ds12 Ds22 Dr2 r2Df 2
26
Method 2
27
Ds2 Dr2 r2Df 2 Ds2 is a linear function of
the quadratics Dr2, Df2 with non-constant
coefficients
28
C sphere of radius a
Ds2 a2Dq 2 a2 sin2q Df 2
29
DeriveD s2 a2Dq 2 a2 sin2q Df 2
30
Method 1
31
Method 1
32
  • NS distance Ds1 aDq
  • EW distance Ds2 rDf a sinq Df
  • Ds2 Ds12 Ds22
  • a2Dq 2 a2 sin2q Df 2

33
Method 2
34
Ds2 a2Dq 2 a2 sin2q Df 2 Ds2 is a linear
function of the quadratics Dq 2, Df 2 with
non-constant coefficients
35
D (r, f)
r is NOT radial distance
36
Two Definitions of r
37
1. Radial definition
38
2. Circumferential definition
C r ? 2p
Ds r ? Df
39
Radial circumferential definitions of r are
consistent iff space is flat
40
E tilted axes
  • x u a v bcosg
  • y v bsing
  • (x1, x2) (u, v)

Ds2 ...
41
Ds2 a2du2 2abcosg dudv b2dv2 Ds2 is a
linear function of the quadratics Du2, Dv2 and
DuDv with cross term
42
Distances Curvature(Qualitative)
43
Distances and curvature (qualitative)
  • Can tell curvature from distances
  • Axially symmetric case
  • Sphere

44
Axaially symmetric
45
D sphere
46
  • Measure distances on the surface (intrinsic)
  • Determine curvature
  • Central idea in differential geometry

47
Riemannian Geometry
48
Riemannian geometry
  • Metric

49
Embedding Sphere
50
Embedding General
51
Cartesian coordinates
Example
52
Distance
Example
53
Curvilinear coordinates
Example
54
Example
55
(No Transcript)
56
Example
57
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58
(No Transcript)
59
Example
60
Embedding General
61
Homogeneous Manifolds
62
Homogeneous manifolds
  • Why homogeneous
  • 3 types
  • closed
  • flat
  • open
  • Robertson-Walker metric

63
Recall 2D homogeneous (surface of sphere)
  • Advantage
  • reduce to flat space if a ? ?
  • Intuitive for 2D "people" one r, one f

64
Flat 2D
Homogeneous curved 2D
65
Flat 3D
Homogeneous curved 3D
66
Cosmology
Spacetime (4)
67
Cosmology(Space only)
  • Three types
  • closed
  • flat
  • open

68
Closed
Flat
69
Together
70
Together
  • 1/a2 k gt 0 closed
  • k 0 flat

71
Open
72
General
73
Most general 3D homogeneous space is describe by
  • One discrete parameter K (1, 0, ?1)
  • One continuous parameter a "size of universe"

74
Reduced radius
"Stuck to grid"
75
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76
F Robertson-Walker metric
77
Questions
  • 1. K ?

78
Other Examples
79
Other examples
  • G. Schwarzschild metric
  • H. Weak fields

80
G Schwarzschild
81
Will NOT derive till laterAccept for the moment
82
  • r ? ? flat
  • r circumferential
  • clocks at different rates
  • gravitational redshift

83
test particle
m
r
M
  • ? ltlt 1 spacetime curvature is small GR NOT
    important
  • ? 1 GR important
  • Black holes

84
H Weak fields
  • Newtonian potential F, F ltlt 1

85
Will NOT derive till laterAccept for the moment
86
Exercise
?
87
Objectives
  • Tell curvature form distances
  • Write down metric in examples
  • General line element
  • Embedding (can be omitted)
  • sphere
  • general

88
Objectives
  • Homogeneous manifolds
  • closed, flat, open
  • Schwarzschild
  • Weak field

89
Acknowledgment
  • This project is supported in part by the Hong
    Kong University Grants Committee (UGC) Teaching
    Development Grants (TDG) 3203005 and 3201032
  • I thank Prof. S.C.Liew for software
  • I thank Prof. M.C.Chu and Dr. S.S.Tong for advice
  • I thank Miss H.Y.Shik for design
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