## Classical Electrodynamics |

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Page 429

3

chapter

special emphasis on the exchange of energy between

the ...

3

**Collisions**between Charged Particles, Energy Loss, and Scattering In thischapter

**collisions**between swiftly moving, charged particles are considered, withspecial emphasis on the exchange of energy between

**collision**partners and onthe ...

Page 443

13.4 Density Effect in

relativistic the observed energy loss is given accurately by (13.44) [or by (13.36) if

m > 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) if

m > 1) for all kinds of particles in all types of media. For ultrarelativistic particles ...

Page 536

The

passes through the atom (b 3 d), and distant

by outside the atom (b > d). The atomic “radius” d can be taken as ao/Z. For the ...

The

**collisions**can be divided into two kinds: close**collisions**where the particlepasses through the atom (b 3 d), and distant

**collisions**where the particle passesby outside the atom (b > d). The atomic “radius” d can be taken as ao/Z. For the ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

5 other sections not shown

### Common terms and phrases

acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge charged particle classical collisions compared component conducting Consequently consider constant coordinates cross section cylinder defined density dependence derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved light limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative relativistic result satisfy scalar scattering shown in Fig shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written