## Classical Electrodynamics |

### From inside the book

Results 1-3 of 69

Page 392

11 , we can immediately deduce the behavior of a

under Lorentz transformations . For neutral particles with no detectable

electromagnetic interactions it is clearly impossible to obtain their relativistic ...

11 , we can immediately deduce the behavior of a

**charged particle**' s momentumunder Lorentz transformations . For neutral particles with no detectable

electromagnetic interactions it is clearly impossible to obtain their relativistic ...

Page 506

The sudden creation of a fast electron in nuclear beta decay , for example , can

be viewed for our purposes as the violent acceleration of a

initially at rest to some final velocity in a very short time interval , or , alternatively ,

as ...

The sudden creation of a fast electron in nuclear beta decay , for example , can

be viewed for our purposes as the violent acceleration of a

**charged particle**initially at rest to some final velocity in a very short time interval , or , alternatively ,

as ...

Page 581

The examples of the last two paragraphs show that the reactive effects of

radiation on the motion of a

the external forces are such that the motion changes appreciably in times of the

order of r ...

The examples of the last two paragraphs show that the reactive effects of

radiation on the motion of a

**charged particle**can be expected to be important ifthe external forces are such that the motion changes appreciably in times of the

order of r ...

### What people are saying - Write a review

We haven't found any reviews in the usual places.

### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

RelativisticParticle Kinematics and Dynamics | 391 |

Copyright | |

8 other sections not shown

### Other editions - View all

### 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 modes 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