## Classical Electrodynamics |

### From inside the book

Results 1-3 of 81

Page 303

If the polarization vector of the incident wave Eo makes an

normal to the plane containing the wave vectors k and ko, the azimuthal

of eul, measured from the plane containing k and ko, is given by y = (m/2) – 6. We

note ...

If the polarization vector of the incident wave Eo makes an

**angle**6 with thenormal to the plane containing the wave vectors k and ko, the azimuthal

**angle**yof eul, measured from the plane containing k and ko, is given by y = (m/2) – 6. We

note ...

Page 457

It is often desirable to use the projected

being made on some convenient plane such as the plane of a photographic

emulsion or a bubble chamber, as shown in Fig. 13.7. For small

to show ...

It is often desirable to use the projected

**angle**of scattering 6', the projectionbeing made on some convenient plane such as the plane of a photographic

emulsion or a bubble chamber, as shown in Fig. 13.7. For small

**angles**it is easyto show ...

Page 458

Or, using (13.107) for (0°), 2 (0°) – 4trN so pu | ln (210ZT*) t (13.111) The mean

square

appreciable energy, the Gaussian will still be peaked at very small forward

Or, using (13.107) for (0°), 2 (0°) – 4trN so pu | ln (210ZT*) t (13.111) The mean

square

**angle**increases linearly with the ... such that the particle does not loseappreciable energy, the Gaussian will still be peaked at very small forward

**angles**.### 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 |

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