## Classical ElectrodynamicsProblems after each chapter |

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Page 443

13.4 Density Effect in Collision Energy

relativistic the observed energy

TJ > 1] for all kinds of particles in all types of media. For ultrarelativistic particles ...

13.4 Density Effect in Collision Energy

**Loss**For particles which are not toorelativistic the observed energy

**loss**is given accurately by (13.44) [or by (13.36) ifTJ > 1] for all kinds of particles in all types of media. For ultrarelativistic particles ...

Page 448

The corresponding relativistic expression without the density effect is, from (13.36

), /JIT\ / — .\2,.. Z r /i m..,A 1 ~l (13.78) We see that the density effect produces a

simplification in that the asymptotic energy

...

The corresponding relativistic expression without the density effect is, from (13.36

), /JIT\ / — .\2,.. Z r /i m..,A 1 ~l (13.78) We see that the density effect produces a

simplification in that the asymptotic energy

**loss**no longer depends on the details...

Page 449

13.5 Energy

incorporated, the upper one being the total energy

energy ...

13.5 Energy

**loss**, including the density effect. The dotted curve is the total energy**loss**without density correction. The solid curves have the density effectincorporated, the upper one being the total energy

**loss**and the lower one theenergy ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

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