| Preface | 7 |
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| Contents | 11 |
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| Acronyms | 14 |
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| A Doubt about the Equivalence Principle | 15 |
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| From Minkowski Spacetime to General Relativity | 19 |
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| 2.1 Semi-Euclidean Coordinate Systems | 19 |
| 2.2 The SE Metric for Uniform Acceleration Is the Only Static SE Metric | 24 |
| 2.3 The Step to General Relativity | 29 |
| 2.4 Weak Field Approximation | 38 |
| 2.5 Geodesic Principle | 50 |
| Gravity as a Force in Special Relativity | 61 |
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| Applying the Strong Equivalence Principle | 64 |
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| The Debate Continues | 71 |
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| A More Detailed Radiation Calculation | 78 |
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| Defining the Radiation from a Uniformly Accelerating Charge | 82 |
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| Energy Conservation for a Uniformly Accelerated Charge | 87 |
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| The Threat to the Equivalence Principle According to Fulton and Rohrlich | 93 |
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| Different Predictions of Special Relativity and General Relativity | 98 |
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| 10.1 Four Cases for Special Relativity | 98 |
| 10.2 Four Cases for General Relativity | 99 |
| 10.3 Conclusion | 100 |
| Derivation of the Lorentz Dirac Equation | 102 |
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| 11.1 Parrott s Derivation | 102 |
| 11.2 Dirac s Derivation | 110 |
| 11.3 Conclusion | 113 |
| 11.4 Self-Force Calculation | 114 |
| Extending the Lorentz Dirac Equation to Curved Spacetime | 116 |
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| 12.1 Equation of Motion of a Charged Particle | 116 |
| 12.2 The Equivalence Principle in All This | 121 |
| 12.3 Conclusions | 134 |
| Static Charge in a Static Spacetime | 136 |
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| A Radiation Detector | 146 |
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| 14.1 Equivalence Principle According to Mould | 146 |
| 14.2 Construction of the Detector and Calculations in General Coordinates | 153 |
| 14.3 Detecting Radiation Where There Is None | 162 |
| 14.4 Conclusion | 164 |
| The Definitive Mathematical Analysis | 166 |
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| 15.1 Static Gravitational Field | 169 |
| 15.2 Relation with Minkowski Spacetime | 172 |
| 15.3 What the Uniformly Accelerated Observer Sees | 176 |
| 15.4 Coordinate Singularity in the SE Metric | 181 |
| 15.5 Some Semi-Euclidean Geometry | 183 |
| 15.6 Redshift in a Uniformly Accelerating SE Frame | 188 |
| 15.7 Interpreting Semi-Euclidean Coordinates | 195 |
| 15.8 Accelerations | 197 |
| 15.9 Fields of a Uniformly Accelerated Charge | 205 |
| 15.9.1 Obtaining the Vector Potential | 205 |
| 15.9.2 Obtaining the Electromagnetic Fields | 213 |
| 15.9.3 Electromagnetic Fields on the Null Surface z + t = 0 | 215 |
| 15.9.4 Fixing up the Fields on the Null Surface | 221 |
| 15.10 Origin of the Delta Function in the Field | 226 |
| 15.11 Conclusions Regarding the Fields | 238 |
| 15.11.1 Fields in Region I | 238 |
| 15.11.2 Fields Along Forward Light Cone of Point on Worldline | 241 |
| 15.11.3 Equivalence of Advanced and Retarded Fields | 243 |
| 15.11.4 Comparing Radiated and Coulomb Fields in Region I | 245 |
| 15.11.5 Situation in Region II | 250 |
| 15.12 Stress Energy Tensor | 254 |
| 15.12.1 Stress Energy Tensor in Accelerating Frame | 255 |
| 15.12.2 Energy Flux | 256 |
| 15.12.3 Boulware s Conclusion about Energy Flow | 261 |
| 15.13 General Conclusions | 261 |
| Interpretation of Physical Quantities in General Relativity | 264 |
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| 16.1 Definition of Energy | 266 |
| 16.2 Lorentz Boost Killing Vector Field in Minkowski Spacetime | 267 |
| 16.3 Killing Vector Field for Static Spacetime | 270 |
| 16.4 Killing Vector Fields for Schwarzschild Spacetime | 271 |
| 16.5 Another Metric | 276 |
| 16.6 And Another Metric | 278 |
| 16.7 Rindler or Elevator Coordinates | 279 |
| 16.8 The Problem with the Poynting Vector | 283 |
| 16.9 Schwarzschild Spacetime Revisited | 291 |
| 16.10 Antithesis of the Present View | 293 |
| Charged Rocket | 298 |
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| 17.1 Preamble | 298 |
| 17.2 Calculation | 307 |
| 17.3 Conclusion | 314 |
| Summary | 316 |
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| Conclusion | 351 |
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| References | 356 |
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| Index | 358 |