Title: PHY 4460 RELATIVITY
1PHY 4460RELATIVITY
- K Young, Physics Department, CUHK
- ?The Chinese University of Hong Kong
2CHAPTER 10MATH OF CURVED SPACE THE METRIC
3Overview
- Distance and metric
- chapter 10 (this one)
- Vectors
- chapter 12
- Differentiation
- chapter 13
- Curvature
- chapter 16
4Objectives
- Tell curvature form distances
- Write down metric in examples
- General line element
- Embedding (can be omitted)
- sphere
- general
5Objectives
- Homogeneous manifolds
- closed, flat, open
- Schwarzschild
- Weak field
6Introduction
- Gravity spacetime curvature
- How do we describe curvature
7Extrinsic
- We can see that the 2D surface of the earth is
curved - By going out of it to 3D and looking down
8Extrinsic
- 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
9Extrinsic
- In relativity N 4 (ie. 31)
- The extra M ? N dimensions are fictitious
- Make sure physics is independent of these
fictitious dimensions
10Intrinsic
- Can we tell surface of earth is curved
- While staying on the surface?
11Intrinsic
- 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
12Embedding vs Intrinsic
13Terminology
14Terminology
- Manifold ? "space" Not to be confused with
space in spacetime
15Coordinates xm
- Need not all have same units
Grid
- Not a vector
- Upper indices
- Lower indices xm do not exist
16- Many coordinate systems possible
- Independence of coordinates
17- Coordinate grid
- Coordinate ? distance
- e.g. polar coordinate Df ? distance
18Central question
- How is distance Ds
- related to the change in coordinates Dxm ?
19Examples ofCoordinates and Distances
20Examples
- A flat space x, y
- B flat space r, f
- C sphere q, f
- D sphere r, f
- E tilted axes
21A (x, y)
Ds2 Dx2 Dy2
22Ds2 Dx2 Dy2 Ds2 is a linear function of the
quadratics Dx2, Dy2
23B (r, f)
x r cosf y r sinf
Ds2 Dr2 r2Df 2
24DeriveD s2 D r2 r2Df 2
25Method 1
Ds2 Ds12 Ds22 Dr2 r2Df 2
26Method 2
27Ds2 Dr2 r2Df 2 Ds2 is a linear function of
the quadratics Dr2, Df2 with non-constant
coefficients
28C sphere of radius a
Ds2 a2Dq 2 a2 sin2q Df 2
29DeriveD s2 a2Dq 2 a2 sin2q Df 2
30Method 1
31Method 1
32- NS distance Ds1 aDq
- EW distance Ds2 rDf a sinq Df
- Ds2 Ds12 Ds22
- a2Dq 2 a2 sin2q Df 2
33Method 2
34Ds2 a2Dq 2 a2 sin2q Df 2 Ds2 is a linear
function of the quadratics Dq 2, Df 2 with
non-constant coefficients
35D (r, f)
r is NOT radial distance
36Two Definitions of r
371. Radial definition
382. Circumferential definition
C r ? 2p
Ds r ? Df
39Radial circumferential definitions of r are
consistent iff space is flat
40E tilted axes
- x u a v bcosg
- y v bsing
- (x1, x2) (u, v)
Ds2 ...
41Ds2 a2du2 2abcosg dudv b2dv2 Ds2 is a
linear function of the quadratics Du2, Dv2 and
DuDv with cross term
42Distances Curvature(Qualitative)
43Distances and curvature (qualitative)
- Can tell curvature from distances
- Axially symmetric case
- Sphere
44Axaially symmetric
45D sphere
46- Measure distances on the surface (intrinsic)
- Determine curvature
- Central idea in differential geometry
47Riemannian Geometry
48Riemannian geometry
49Embedding Sphere
50Embedding General
51Cartesian coordinates
Example
52Distance
Example
53Curvilinear coordinates
Example
54Example
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56Example
57(No Transcript)
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59Example
60Embedding General
61Homogeneous Manifolds
62Homogeneous manifolds
- Why homogeneous
- 3 types
- closed
- flat
- open
- Robertson-Walker metric
63Recall 2D homogeneous (surface of sphere)
- Advantage
- reduce to flat space if a ? ?
- Intuitive for 2D "people" one r, one f
64Flat 2D
Homogeneous curved 2D
65Flat 3D
Homogeneous curved 3D
66Cosmology
Spacetime (4)
67Cosmology(Space only)
- Three types
- closed
- flat
- open
68Closed
Flat
69Together
70Together
- 1/a2 k gt 0 closed
- k 0 flat
71Open
72General
73Most general 3D homogeneous space is describe by
- One discrete parameter K (1, 0, ?1)
- One continuous parameter a "size of universe"
74Reduced radius
"Stuck to grid"
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76F Robertson-Walker metric
77Questions
78Other Examples
79Other examples
- G. Schwarzschild metric
- H. Weak fields
80G Schwarzschild
81Will NOT derive till laterAccept for the moment
82- r ? ? flat
- r circumferential
- clocks at different rates
- gravitational redshift
83test particle
m
r
M
- ? ltlt 1 spacetime curvature is small GR NOT
important - ? 1 GR important
- Black holes
84H Weak fields
- Newtonian potential F, F ltlt 1
85Will NOT derive till laterAccept for the moment
86Exercise
?
87Objectives
- Tell curvature form distances
- Write down metric in examples
- General line element
- Embedding (can be omitted)
- sphere
- general
88Objectives
- Homogeneous manifolds
- closed, flat, open
- Schwarzschild
- Weak field
89Acknowledgment
- 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