ph5011 general relativity dr hongsheng zhao shortened/expanded from notes of md [email protected]...
TRANSCRIPT
PH5011
General Relativity
Dr HongSheng Zhao shortened/expanded from notes of MD
Martinmas 2012/2013
0.1 Summation convention
0 General issues
2
pairwise indices imply sum
0.2 Indices
dimension of coordinate space
Apart from a few exceptions,upper and lower indices
are to be distinguished thoroughly
1. Basis (not examined) intro. tensor and Coordinates transformation (exam).
2. Tensor operations all examinable.3. Mechanics classical NOT exam.4. Mechanics in curved space NOT exam.5. Special Rela. NOT exam.6. General Rela. (Einstein Eq.) exam.7. Application of GR Examinable: FRW (p1-6), Schwarzschild (p1-4), Tutorials (1,2,3). Adv. (1p, for intuition)
To Exam Or Not To Exam
3
1.1 Basis and coordinates
1 Curvilinear coordinates
set of basis vectors spans tangent space at⤿
in general, the basis vectors depend on
described by set of coordinates location
infinitesimal displacement in space on variation of coordinategiven by line element
≡ basis vector related to coordinate
coordinate line given by for all
tangent vector at
3
1 Curvilinear coordinates1.1 Basis and coordinates
4
1 Curvilinear coordinates
Example A: Cartesian coordinates (I)
1 Curvilinear coordinates1.1 Basis and coordinates
5
1 Curvilinear coordinates
Example B: Constant, non-orthogonal system (I)
1.2 Reciprocal basis
Kronecker-delta
orthonormal basis
orthogonal basis
6
1 Curvilinear coordinates
construction:
orthogonality
normalization for
for
for
1 Curvilinear coordinates1.2 Reciprocal basis
7
1 Curvilinear coordinates
Special case: 3 dimensions
Example A: Cartesian coordinates (II)
1 Curvilinear coordinates
8
1 Curvilinear coordinates1.2 Reciprocal basis
⤿
Example B: Constant, non-orthogonal system (II)
1 Curvilinear coordinates
9
1 Curvilinear coordinates1.2 Reciprocal basis
⤿
1.3 Metric1 Curvilinear coordinates
10
⤿
coefficients of metric tensor (→ 1.5)
as matrix
symmetry:
1 Curvilinear coordinates1.3 Metric
11
Examples A+B: Cartesian & non-orthogonal constant basis (III)
⤿
⤿
1 Curvilinear coordinates
12
length of curve given by
1.3 Metric
parametric representation of curve
1 Curvilinear coordinates1.3 Metric
13
Example: Length of equator in spherical coordinates
in
one only needs to consider :
⤿
use parameter along the azimuth
one full turn for and
⤿
1.3 Metric1 Curvilinear coordinates
equivalent to the condition for the inverse matrix
which fulfill ,
With the reciprocal basis ,
one defines reciprocal components of the metric tensor
14
1.3 Metric1 Curvilinear coordinates
metric tensor
orthonormality condition
“lowers index”
“raises index”
⤿
15
1.4 Vector fields1 Curvilinear coordinates
mathematics: vector fieldphysics: vector (field)
covariant components
contravariant components(→ 1.6)
“raising/lowering indices”
vector components defined by means of basis vectors
16
1.5 Tensor fields1 Curvilinear coordinates
tensor is multi-dimensional generalization of vector
mathematics: tensor fieldphysics: tensor (field)
behaves like a vector with respect to each of the vector spaces
17
product of vector spaces
tensor of rank 2 square matrixtensor of rank 1 tensor of rank 0
tensor of rank 3 cube
vectorscalar
........
rank of tensor
1 Curvilinear coordinates
18
1.5 Tensor fields
basis vectors apply to each of the vector spaces
⤿
covariant components
contravariant components
mixed components
1.5 Tensor fields1 Curvilinear coordinates
19
Example: Rank-2 tensor
⤿
Coincidentally, with the matrix product
For Cartesian coordinates:
1.6 Coordinate transformations1 Curvilinear coordinates
20
consider different set of coordinates
(chain rule)
different coordinate systems describe same locations
⤿
⤿
1 Curvilinear coordinates
21
covariantcontravariant
derivativesdifferentials
components transform like coordinate {}
1.6 Coordinate transformations
vector fields
tensor fields
⤿
⤿
1.6 Coordinate transformations1 Curvilinear coordinates
22
1 Curvilinear coordinates
Proof: are covariant components of a tensor
⤿
1.7 Affine connection1 Curvilinear coordinates
in general, basis vectors depend on the coordinates
derivative of basis vector written in basis
23
affine connection (Christoffel symbol)
derivative of reciprocal basis vector:
⤿
1 Curvilinear coordinates1.7 Affine connection
1 Curvilinear coordinates
24
Example C: Spherical coordinates (IV)
⤿
⤿
1 Curvilinear coordinates1.7 Affine connection
1 Curvilinear coordinates
25
Example C: Spherical coordinates (IV) [continued]
⤿
⤿
⤿
1 Curvilinear coordinates1.7 Affine connection
1 Curvilinear coordinates
given that
the Christoffel symbols can be expressed by means
of the components of the metric tensor and their derivatives
26
1 Curvilinear coordinates
27
1 Curvilinear coordinates1.7 Affine connection
Proof:
⤿ (I)
(II)
(III)
(II) + (III) - (I) :
⤿
2 Tensor analysis
derivative:
28
vector field
both the vector components and the basis vectorsdepend on the coordinates
define covariant derivative of a contravariant vector component
as so that
2.1 Covariant derivative
2 Tensor analysis2.1 Covariant derivative
derivatives transform as
⤿ can be considered the covariant components
of the vector
29
covariant components of a vector
(gradient)
form components of a tensor, not
2 Tensor analysis2.1 Covariant derivative
covariant componentscontravariant components
30
for eachupper
lowerindex , add {{ }
takes place of in orwhere
covariant derivatives of tensor components
31
2 Tensor analysis2.1 Covariant derivative
Covariant derivative of 2nd-rank tensor
⤿
2.2 Riemann tensor2 Tensor analysis
with the Riemann (curvature) tensor
(not intended to be memorized)
order of 2nd covariant derivatives of vector
is not commutative
with
⤿
and
, but
32
2 Tensor analysis
33
2.2 Riemann tensor
Riemann tensor has two pairs of indices and is
antisymmetric in the indices of each pair
[ [
symmetric in exchanging the pairs
Moreover,
(1st Bianchi identity)
(2nd Bianchi identity)
2 Tensor analysis
34
2.2 Riemann tensor
Proof:
The scalar product of two vectors is a scalar
⤿
On the other hand
⤿
(Riemann curvature tensor is antisymmetric in first two indices)
2 Tensor analysis
35
2.3 Einstein tensor
must relate to Riemann tensor
matches required conditions⤿
only a single non-vanishing contraction (up to a sign)
(Ricci tensor)
with next-level contraction
(Ricci scalar)
2nd-rank curvature tensor fulfilling
3 Review: Classical Mechanics3.1 Principle of stationary action
action
Fermat’s principle (optics)Feynman’s path integral (QM)
(Hamilton’s) principle of stationary action
for : kinetic energypotential energy
Mechanical system completely described by
(Lagrangian)coordinatevelocitytime
36
(Euler-) Lagrange equations⤿
Example: 1D harmonic oscillator (I)
⤿
⤿
⤿
3 Classical mechanics3.1 Principle of stationary action
37
(geodesic equation, assume ⤿⤿= s )
4.1 Principle of stationary paths
47
stationary path between two points(e.g. path length is locally shortest)
Christoffel symbols(affine connection)
4 Intro: Mech. in curved space
Path length ds = G d⤿ , stationary path means
48
4 Mechanics in curved space4.1 Stationary paths
Define
⤿
Constant L factored out of derivatives. Write derivative as dot, if we define t = s = ⤿
⤿
⤿
L resembles Lagrangian for a free particle of mass m in curved space
with and
⤿
(Euler-Lagrange equations)
⤿
⤿
↳
}⤿
44
4 Mechanics in curved space4.1 Stationary paths
4 Mechanics in curved space
49
4.1 Stationary paths
Eq. of motion along geodesics, ⤿⤿= s, or in shorthand:
based on Newton’s law purely space geometry
(geodesic equation)
4 Mechanics in curved space
4.2 Geodesics as parallel transport
•moving along geodesics means to keep the same direction•geodesics form “straight lines”
46
= tangent unit vector to a curve
i.e.
is geodesic if unit tangent vector is parallelly transported
if all do not depend on ⤿
4.3 Conserved momentum pk dpk/d⤿=0 if the metric g independent of qk
4 Mechanics in curved space
50
(geodesic equation)
5 Review: Special Relativity
54
5.1 Minkowski space
“inertial system”force-free particles move uniformly
all reference frames moving uniformly with respect to an inertial system are inertial system themselves
“reference frame”defines coordinate origin and motion
“event” described by time and location
laws of physics assume the same form in all inertial systems
55
5 Special Relativity5.1 Minkowski space
describes distance in four-dimensional space⤿depend on reference frameboth and whereas
homogeneity and isotropy of space and time
⤿ invariance of
⤿
⤿ along light rays:
for all reference frames
invariance of speed of light
56
5 Special Relativity5.1 Minkowski space
Latin indices
Greek indices
use 4-dimensional vectors
flat three-dimensional space described by cartesian coordinates
⤿
photons trace null geodesics between eventsdefines light cone 45° opening angle in
5.2 Light cone5 Special Relativity
57
or: “causality and the finite speed of light”
instantaneous knowledge of interactionnon-relativistic theories:
light cone widens, all events get into causal contact
:
invariance ofcategorization holds irrespective of coordinate system and reference frame⤿
outside light cone‘elsewhere’, no causal connection
inside light conemassive particles move on time-like geodesics
5.3 Proper time5 Special Relativity
58
time shown on clock
⤿ proper time
invariance of ⤿
⤿
(moving clock observed “t” appears big )so that
along worldline of clock with attached rest frame
5 Special Relativity
59
5.4 Relativistic mechanicsdefine 4-velocity as
⤿
⤿
⤿(as anticipated for inertial system)
known: free particle moves along geodesic
⤿ [ all ]
5 Special Relativity
( ) non-relativistic limit
60
⤿⤿⤿⤿
5.4 Relativistic mechanics
(matches invariance of )ansatz:
relativistic action
5.4 Relativistic mechanics5 Special Relativity
conjugate momentum
61
energy
⤿
(relativistic Hamilton-Jacobi equation)
with
⤿
(sign in spatial part due to in metric)
components of stress tensor
provides relation between the forces and the cross-sections these are exerted on
forcearea of cross-sectionnormal to cross-section
5.5 Energy-momentum tensor5 Special Relativity
62
for fluid in thermodynamic equilibrium:(no shear stresses)
pressure
energy-momentumtensor
in fluid rest frame:
mass density
complement to
energy densitymomentum density
stress
5 Special Relativity5.5 Energy-momentum tensor
63
non-relativistic limit:
(continuity equation)
(↔ Newton’s law)
6 General Relativity
64
6.1 Principlesexperiments cannot distinguish between:
• virtual forces present in non-inertial frames• true forces
gravitation can be described byspace-time metric
⤿
gravitation becomes property of space-time with particles moving on geodesics⤿
local free-falling frame is an inertial frame, where free particles are on straight lines and
→ Einstein’s field equationsonly remaining issue: relation between and Newton’s law
6 General Relativity6.1 Principles
The laws of physics are the same for all observers,irrespective of their motion
Physical laws take the same covariant form in all coordinate systems
We live in a 4-dimensional curved metric space-time
Particles move along geodesics
The laws of Special Relativity apply locallyfor all non-accelerated (inertial) observers
The curvature follows the energy-momentum tensoras described by Einstein’s field equations
General Relativity summarized in 6 points
65
66
6 General Relativity
6.2 Einstein’s field equations
independence on choice of coordinatesformulate theory by means of tensor fields⤿
if non-relativistic limit reproduces Newton’s law,this is not necessarily the only possible theory,
but the most simple one that conforms to the principles⤿
⤿ ?
(energy-momentum tensor)
matter is completely described by 2nd-rank tensor
description of curvature by 2nd-rank tensor
(Einstein tensor)
6 General Relativity6.2 Einstein’s field equations
67
Einstein’s field equations:
non-relativistic limit ( ):
dominating
,
⤿
6 General Relativity6.2 Einstein’s field equations
Newton:
⤿
⤿
⤿with
⤿
68
6 General Relativity6.2 Einstein’s field equations
[note: Einstein’s orignal sign convention for the Ricci tensor differs from ours]69
6 General Relativity
theories modifying the law of gravity provide alternative models
6.3 Cosmological constant
70
negligible correction, unless huge length scales are considered
modified Einstein tensor
also fulfills
(dark) “vacuum” energy ??effective repulsion
measurements suggest
Solar neighbourhoodbaryonic matter in the Universe
71
6 General Relativity
6.4 Time and distanceLaws of physics — described by tensors — do not depend on coordinates
coordinates do not have immediate physical meaning⤿⤿ What is the time and distance?
can be locally transformed to
are not completely arbitrary
⤿ matrix with eigenvalues of
corresponding to 1 time-like and 3 space-like coordinateshave signs
⤿
6 General Relativity6.4 Time and distance
cannot define spatial distance by means of for neighbouring events at the same time
⤿
in general, the relation between the proper time interval and
depends on the location
time interval between two events at the same locationgiven by
⤿ proper time
72
coordinate transformation can always provide(at cost of time-dependent )
(synchronized reference frame)everywhere
coordinate line of (i.e. ) is geodesic
6 General Relativity6.5 Synchronisation
(with regard to time coordinate, but measured depends on location)global synchronisation possible⤿if
76
6.5 Synchronisation (e.g. FRW cosmology)
Challenge: prove this
110
7 GR Applications
7. Satellites: GPS orbit Earth ~ stars orbit BHBeepers on sat. are Doppler/Gravitational-shifted, time delayed
112
7 Consequences7. Satellite navigation
GPS satellites perform two orbits per sidereal day
GPS clocks are shipped with “factory offset” to compensate
in total, GPS clock appears to run faster by
⤿ ,
Doppler shift (transverse motion)
per day
gravitational potential
per day
per day
7 Consequences7.1 Relativistic Kepler problem
87
Perihelion shift of the planets in the Solar system
semi-major semi-major axisaxis
a a [AU][AU]
orbital orbital periodperiod
P P [yr][yr]
eccentriciteccentricityyεε
perihelion perihelion shiftshift
per centuryper century
Mercury
☿ 0.39 0.25 0.206 43˝
Venus ♀ 0.72 0.62 0.0068 8.6˝
Earth ♁ 1 1 0.0167 3.8˝
Mars ♂ 1.5 1.88 0.0933 1.4˝
Jupiter ♃ 5.2 11.9 0.048 0.06˝
Saturn ♄ 9.5 29.5 0.056 0.01˝
Uranus ♅ 19 84 0.046 0.002˝
Neptune
♆ 30 165 0.010 0.0008˝
(essentially inversely proportional to a5/2)
7 Consequences7.1 Relativistic Kepler problem
86
90
7 Consequences7.2 Bending of light
asymptotics
⤿ total deflection ⤿
Deflection of light by gravity (1915)
α =4GMc2ξ1.″7
measurable at Solar limb: α =
bending angle
92
93
7 Consequences7.2 Bending of light
"The present eclipse expeditions may for the first time demonstrate theweight of light; or they may confirm Einstein's weird theory of non-Euclidean space; orthey may lead to a result of yet more far-reaching
consequences -- no deflection.""The generalized relativity theory is a most profound theory of
Nature,embracing almost all the phenomena of physics."
(Sir) Arthur Stanley Eddington
Negative of one of the photographic plates
taken by the British expedition to Sobral (Brazil)
during the total Solar Eclipse of 29 May 1919© The Royal Society
The British expeditions to Sobral (Brazil) and the island of Principe
to observe the total Solar Eclipse of 29 May 1919
95
7 Consequences7.2 Bending of light
99
Notes about gravitational microlensing dated to 1912on two pages of Einstein’s scratch notebook
I−
I+
ξη
side view
7 Consequences7.2 Bending of light
Images by a gravitational lens
96
⤿
with (angular Einstein radius)
(two images)⤿
6˝
(animation by Daniel Kubas, ESO)
98
7 Consequences7.2 Bending of light
bending of light of stars due to intervening foreground stars
image distortion leads to observable transient brightening
images cannot be resolved⤿
within the Milky Way
⤿
The chance isone in a million !
B. Paczyński 1986, ApJ 304, 1
7 Consequences7.2 Bending of light
100
First reported microlensing event
MACHO LMC#1
Nature 365, 621 (October 1993)
7 Consequences7.2 Bending of light
101
Astronomy & Geophysics Vol. 47
(June 2006)
7 Consequences7.2 Bending of light
102
A Sample of Advanced Material: Geodesics around Black Hole Metric