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- Half-title
- Title
- Copyright
- Contents
- Preface
- Notation
- I. Special Relativity
- 1 Introduction: Inertial systems and the Galilei invariance of Classical Mechanics
- 1.1 Inertial systems
- 1.2 Invariance under translations
- 1.3 Invariance under rotations
- 1.4 Invariance under Galilei transformations
- 1.5 Some remarks on the homogeneity of time
- Exercises
- 2 Light propagation in moving coordinate systems and Lorentz transformations
- 2.1 The Michelson experiment
- 2.2 The Lorentz transformations
- 2.3 Some properties of Lorentz transformations
- Exercises
- 3 Our world as a Minkowski space
- 3.1 The concept of Minkowski space
- 3.2 Four-vectors and light cones
- 3.3 Measuring length and time in Minkowski space
- 3.4 Two thought experiments
- 3.4.1 A rod moving through a tube
- 3.4.2 The twin paradox
- 3.5 Causality, and velocities larger than that of light
- Exercises
- 4 Mechanics of Special Relativity
- 4.1 Kinematics
- 4.2 Equations of motion
- 4.3 Hyperbolic motion
- 4.4 Systems of particles
- Exercises
- 5 Optics of plane waves
- 5.1 Invariance of phase and null vectors
- 5.2 The Doppler effect – shift in the frequency of a wave
- 5.3 Aberration – change in the direction of a light ray
- 5.4 The visual shape of moving bodies
- 5.5 Reflection at a moving mirror
- 5.6 Dragging of light within a fluid
- Exercises
- 6 Four-dimensional vectors and tensors
- 6.1 Some definitions
- 6.2 Tensor algebra
- 6.3 Symmetries of tensors
- 6.4 Algebraic properties of second rank tensors
- 6.5 Tensor analysis
- Exercises
- 7 Electrodynamics in vacuo
- 7.1 The Maxwell equations in three-dimensional notation
- 7.2 Current four-vector, four-potential, and the retarded potentials
- 7.3 Field tensor and the Maxwell equations
- 7.4 Poynting’s theorem, Lorentz force, and the energy-momentum tensor
- 7.5 The variational principle for the Maxwell equations
- Exercises
- 8 Transformation properties of electromagnetic fields: examples
- 8.1 Current and four-potential
- 8.2 Field tensor and energy-momentum tensor
- Exercises
- 9 Null vectors and the algebraic properties of electromagnetic field tensors
- 9.1 Null tetrads and Lorentz transformations
- 9.2 Self-dual bivectors and the electromagnetic field tensor
- 9.3 The algebraic classification of electromagnetic fields
- 9.4 The physical interpretation of electromagnetic null fields
- Exercises
- 10 Charged point particles and their field
- 10.1 The equations of motion of charged test particles
- 10.2 The variational principle for charged particles
- 10.3 Canonical equations
- 10.4 The field of a charged particle in arbitrary motion
- 10.5 The equations of motion of charged particles – the self-force
- Exercises
- Further reading for Chapter 10
- 11 Pole-dipole particles and their field
- 11.1 The current density
- 11.2 The dipole term and its field
- 11.3 The force exerted on moving dipoles
- Exercises
- 12 Electrodynamics in media
- 12.1 Field equations and constitutive relations
- 12.2 Remarks on the matching conditions at moving surfaces
- 12.3 The energy-momentum tensor
- Exercises
- 13 Perfect fluids and other physical theories
- 13.1 Perfect fluids
- 13.2 Other physical theories – an outlook
- II. Riemannian geometry
- 14 Introduction: the force-free motion of particles in Newtonian mechanics
- 14.1 Coordinate systems
- 14.2 Equations of motion
- 14.3 The geodesic equation
- 14.4 Geodesic deviation
- Exercise
- 15 Why Riemannian geometry?
- 16 Riemannian space
- 16.1 The metric
- 16.2 Geodesics and Christoffel symbols
- 16.3 Coordinate transformations
- 16.4 Special coordinate systems
- 16.5 The physical meaning and interpretation of coordinate systems
- Exercises
- Further reading for Chapter 16
- 17 Tensor algebra
- 17.1 Scalars and vectors
- 17.2 Tensors and other geometrical objects
- 17.3 Algebraic operations with tensors
- 17.4 Tetrad and spinor components of tensors
- Exercises
- Further reading for Section 17.4
- 18 The covariant derivative and parallel transport
- 18.1 Partial and covariant derivatives
- 18.2 The covariant differential and local parallelism
- 18.3 Parallel displacement along a curve and the parallel propagator
- 18.4 Fermi–Walker transport
- 18.5 The Lie derivative
- Exercises
- Further reading for Chapter 18
- 19 The curvature tensor
- 19.1 Intrinsic geometry and curvature
- 19.2 The curvature tensor and global parallelism of vectors
- 19.3 The curvature tensor and second derivatives of the metric tensor
- 19.4 Properties of the curvature tensor
- 19.5 Spaces of constant curvature
- Exercises
- Further reading for Chapter 19
- 20 Differential operators, integrals and integral laws
- 20.1 The problem
- 20.2 Some important differential operators
- 20.3 Volume, surface and line integrals
- 20.4 Integral laws
- 20.5 Integral conservation laws
- Further reading for Chapter 20
- 21 Fundamental laws of physics in Riemannian spaces
- 21.1 How does one find the fundamental physical laws?
- 21.2 Particle mechanics
- 21.3 Electrodynamics in vacuo
- 21.4 Geometrical optics
- 21.5 Thermodynamics
- 21.6 Perfect fluids and dust
- 21.7 Other fundamental physical laws
- Exercises
- Further reading for Chapter 21
- III. Foundations of Einstein’s theory of gravitation
- 22 The fundamental equations of Einstein’s theory of gravitation
- 22.1 The Einstein field equations
- 22.2 The Newtonian limit
- 22.3 The equations of motion of test particles
- Further reading for Section 22.3
- 22.4 A variational principle for Einstein’s theory
- 23 The Schwarzschild solution
- 23.1 The field equations
- 23.2 The solution of the vacuum field equations
- 23.3 General discussion of the Schwarzschild solution
- 23.4 The motion of the planets and perihelion precession
- 23.5 The propagation of light in the Schwarzschild field
- 23.6 Further aspects of the Schwarzschild solution
- 23.7 The Reissner–Nordström solution
- Exercises
- 24 Experiments to verify the Schwarzschild metric
- 24.1 Some general remarks
- 24.2 Perihelion precession and planetary orbits
- 24.3 Light deflection by the Sun
- 24.4 Redshifts
- 24.5 Measurements of the travel time of radar signals (time delay)
- 24.6 Geodesic precession of a top
- Further reading for Chapter 24
- 25 Gravitational lenses
- 25.1 The spherically symmetric gravitational lens
- 25.2 Galaxies as gravitational lenses
- Exercise
- 26 The interior Schwarzschild solution
- 26.1 The field equations
- 26.2 The solution of the field equations
- 26.3 Matching conditions and connection to the exterior Schwarzschild solution
- 26.4 A discussion of the interior Schwarzschild solution
- Exercises
- IV. Linearized theory of gravitation, far fields and gravitational waves
- 27 The linearized Einstein theory of gravity
- 27.1 Justification for a linearized theory and its realm of validity
- 27.2 The fundamental equations of the linearized theory
- 27.3 A discussion of the fundamental equations and a comparison with special-relativistic electrodyn
- 27.4 The far field due to a time-dependent source
- 27.5 Discussion of the properties of the far field (linearized theory)
- 27.6 Some remarks on approximation schemes
- Further reading for Section 27.6
- Exercise
- 28 Far fields due to arbitrary matter distributions and balance equations for momentum and angular m
- 28.1 What are far fields?
- 28.2 The energy-momentum pseudotensor for the gravitational field
- 28.3 The balance equations for momentum and angular momentum
- 28.4 Is there an energy law for the gravitational field?
- Further reading for Chapter 28
- 29 Gravitational waves
- 29.1 Are there gravitational waves?
- 29.2 Plane gravitational waves in the linearized theory
- 29.3 Plane waves as exact solutions of Einstein’s equations
- 29.4 The experimental evidence for gravitational waves
- Exercises
- 30 The Cauchy problem for the Einstein field equations
- 30.1 The problem
- 30.2 Three-dimensional hypersurfaces and reduction formulae for the curvature tensor
- 30.3 The Cauchy problem for the vacuum field equations
- 30.4 The characteristic initial value problem
- 30.5 Matching conditions at the boundary surface of two metrics
- V. Invariant characterization of exact solutions
- 31 Preferred vector fields and their properties
- 31.1 Special simple vector fields
- 31.2 Timelike vector fields
- 31.3 Null vector fields
- Exercises
- 32 The Petrov classification
- 32.1 What is the Petrov classification?
- 32.2 The algebraic classification of gravitational fields
- 32.3 The physical interpretation of degenerate vacuum gravitational fields
- Exercises
- 33 Killing vectors and groups of motion
- 33.1 The problem
- 33.2 Killing vectors
- 33.3 Killing vectors of some simple spaces
- 33.4 Relations between the curvature tensor and Killing vectors
- 33.5 Groups of motion
- 33.6 Killing vectors and conservation laws
- Exercises
- 34 A survey of some selected classes of exact solutions
- 34.1 Degenerate vacuum solutions
- 34.2 Vacuum solutions with special symmetry properties
- 34.3 Perfect fluid solutions with special symmetry properties
- Exercises
- VI. Gravitational collapse and black holes
- 35 The Schwarzschild singularity
- 35.1 How does one examine the singular points of a metric?
- 35.2 Radial geodesics near r = 2M
- 35.3 The Schwarzschild solution in other coordinate systems
- 35.4 The Schwarzschild solution as a black hole
- Exercises
- 36 Gravitational collapse – the possible life history of a spherically symmetric star
- 36.1 The evolutionary phases of a spherically symmetric star
- 36.2 The critical mass of a star
- 36.3 Gravitational collapse of spherically symmetric dust
- Further reading for Chapter 36
- 37 Rotating black holes
- 37.1 The Kerr solution
- 37.2 Gravitational collapse – the possible life history of a rotating star
- 37.3 Some properties of black holes
- 37.4 Are there black holes?
- Further reading for Chapter 37
- 38 Black holes are not black – Relativity Theory and Quantum Theory Theory and Quantum Theory
- 38.1 The problem
- 38.2 Unifled quantum field theory and quantization of the gravitational field
- 38.3 Semiclassical gravity
- 38.4 Quantization in a given classical gravitational field
- 38.5 Black holes are not black – the thermodynamics of black holes
- Further reading for Chapter 38
- 39 The conformal structure of infinity
- 39.1 The problem and methods to answer it
- 39.2 Infinity of the three-dimensional Euclidean space (E3)
- 39.3 The conformal structure of Minkowski space
- 39.4 Asymptotically flat gravitational fields
- 39.5 Examples of Penrose diagrams
- Exercises
- VII. Cosmology
- 40 Robertson–Walker metrics and their properties
- 40.1 The cosmological principle and Robertson–Walker metrics
- 40.2 The motion of particles and photons
- 40.3 Distance definitions and horizons
- 40.4 Some remarks on physics in closed universes
- Exercises
- 41 The dynamics of Robertson–Walker metrics and the Friedmann universes
- 41.1 The Einstein field equations for Robertson–Walker metrics
- 41.2 The most important Friedmann universes
- 41.3 Consequences of the field equations for models with arbitrary equation of state having positive
- Exercises
- 42 Our universe as a Friedmann model
- 42.1 Redshift and mass density
- 42.2 The earliest epochs of our universe and the cosmic background radiation
- 42.3 A Schwarzschild cavity in the Friedmann universe
- 43 General cosmological models
- 43.1 What is a cosmological model?
- 43.2 Solutions of Bianchi type I with dust
- 43.3 The Gödel universe
- 43.4 Singularity theorems
- Exercises
- Further reading for Chapter 43
- Bibliography
- Alternative textbooks on relativity and useful review volumes
- Monographs and research articles
- Index
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