| A Doubt about the Equivalence Principle | p. 1 |
| From Minkowski Spacetime to General Relativity | p. 5 |
| Semi-Euclidean Coordinate Systems | p. 5 |
| The SE Metric for Uniform Acceleration Is the Only Static SE Metric | p. 10 |
| The Step to General Relativity | p. 15 |
| Weak Field Approximation | p. 24 |
| Geodesic Principle | p. 36 |
| Gravity as a Force in Special Relativity | p. 47 |
| Applying the Strong Equivalence Principle | p. 51 |
| The Debate Continues | p. 59 |
| A More Detailed Radiation Calculation | p. 67 |
| Defining the Radiation from a Uniformly Accelerating Charge | p. 71 |
| Energy Conservation for a Uniformly Accelerated Charge | p. 77 |
| The Threat to the Equivalence Principle According to Fulton and Rohrlich | p. 83 |
| Different Predictions of Special Relativity and General Relativity | p. 89 |
| Four Cases for Special Relativity | p. 89 |
| Four Cases for General Relativity | p. 90 |
| Conclusion | p. 91 |
| Derivation of the Lorentz-Dirac Equation | p. 93 |
| Parrott's Derivation | p. 93 |
| Dirac's Derivation | p. 101 |
| Conclusion | p. 104 |
| Self-Force Calculation | p. 105 |
| Extending the Lorentz-Dirac Equation to Curved Spacetime | p. 107 |
| Equation of Motion of a Charged Particle | p. 107 |
| The Equivalence Principle in All This | p. 112 |
| Conclusions | p. 125 |
| Static Charge in a Static Spacetime | p. 127 |
| A Radiation Detector | p. 137 |
| Equivalence Principle According to Mould | p. 137 |
| Construction of the Detector and Calculations in General Coordinates | p. 144 |
| Detecting Radiation Where There Is None | p. 153 |
| Conclusion | p. 155 |
| The Definitive Mathematical Analysis | p. 157 |
| Static Gravitational Field | p. 160 |
| Relation with Minkowski Spacetime | p. 163 |
| What the Uniformly Accelerated Observer Sees | p. 167 |
| Coordinate Singularity in the SE Metric | p. 172 |
| Some Semi-Euclidean Geometry | p. 174 |
| Redshift in a Uniformly Accelerating SE Frame | p. 179 |
| Interpreting Semi-Euclidean Coordinates | p. 186 |
| Accelerations | p. 188 |
| Fields of a Uniformly Accelerated Charge | p. 196 |
| Obtaining the Vector Potential | p. 196 |
| Obtaining the Electromagnetic Fields | p. 204 |
| Electromagnetic Fields on the Null Surface z + t = 0 | p. 206 |
| Fixing up the Fields on the Null Surface | p. 212 |
| Origin of the Delta Function in the Field | p. 217 |
| Conclusions Regarding the Fields | p. 229 |
| Fields in Region I | p. 229 |
| Fields Along Forward Light Cone of Point on Worldline | p. 232 |
| Equivalence of Advanced and Retarded Fields | p. 234 |
| Comparing Radiated and Coulomb Fields in Region I | p. 236 |
| Situation in Region II | p. 241 |
| Stress-Energy Tensor | p. 245 |
| Stress-Energy Tensor in Accelerating Frame | p. 246 |
| Energy Flux | p. 247 |
| Boulware's Conclusion about Energy Flow | p. 252 |
| General Conclusions | p. 252 |
| Interpretation of Physical Quantities in General Relativity | p. 255 |
| Definition of Energy | p. 257 |
| Lorentz Boost Killing Vector Field in Minkowski Spacetime | p. 258 |
| Killing Vector Field for Static Spacetime | p. 261 |
| Killing Vector Fields for Schwarzschild Spacetime | p. 262 |
| Another Metric | p. 267 |
| And Another Metric | p. 269 |
| Rindler or Elevator Coordinates | p. 270 |
| The Problem with the Poynting Vector | p. 274 |
| Schwarzschild Spacetime Revisited | p. 282 |
| Antithesis of the Present View | p. 284 |
| Charged Rocket | p. 289 |
| Preamble | p. 289 |
| Calculation | p. 298 |
| Conclusion | p. 305 |
| Summary | p. 307 |
| Conclusion | p. 343 |
| References | p. 349 |
| Index | p. 351 |
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