## Classical ElectrodynamicsProblems after each chapter |

### From inside the book

Results 1-3 of 79

Page 457

ZA mc) It is often desirable to use the projected

projection 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

ZA mc) It is often desirable to use the projected

**angle**of scattering 6', theprojection 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

**angles**it is easy ...Page 458

107) for (fl2), )f (13.111) pv The mean square

thickness /. But for reasonable thicknesses such that the particle does not lose

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

107) for (fl2), )f (13.111) pv The mean square

**angle**increases linearly with thethickness /. But for reasonable thicknesses such that the particle does not lose

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

**angles**.Page 459

13.8 Multiple and single scattering distributions of projected

of plural scattering (a ~ 2-3) the dotted curve indicates the smooth transition from

the small-

13.8 Multiple and single scattering distributions of projected

**angle**. In the regionof plural scattering (a ~ 2-3) the dotted curve indicates the smooth transition from

the small-

**angle**multiple scattering (approximately Gaussian in shape) to the ...### What people are saying - Write a review

#### LibraryThing Review

User Review - barriboy - LibraryThingA soul crushing technical manual written by a sadist that has served as the right of passage for physics PhDs since the dawn of time. Every single one of my professors studied this book, and every ... Read full review

#### LibraryThing Review

User Review - aproustian - LibraryThing"Jackson E&M is about learning how to approximate reliably...the entire book, with few exceptions, is a mathematical discussion on how to solve [the same] 4 problems for different boundary conditions." Read full review

### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

4 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 coefficients 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 shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written