## Classical Electrodynamics |

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Page 22

1.8 This expression for

high fields “must” contain considerable

thing about (1.55). The

volume ...

1.8 This expression for

**energy**density is intuitively reasonable, since regions ofhigh fields “must” contain considerable

**energy**. There is perhaps one puzzlingthing about (1.55). The

**energy**density is positive definite. Consequently itsvolume ...

Page 448

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

), (#) _ (-e)'o. in (o) - | (13.78) dar/b-a co a (00) 2 We see that the density effect

produces a simplification in that the asymptotic

on ...

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

), (#) _ (-e)'o. in (o) - | (13.78) dar/b-a co a (00) 2 We see that the density effect

produces a simplification in that the asymptotic

**energy**loss no longer dependson ...

Page 537

(a) Calculate the cross sections for

collisions (write them as functions of Q/I as far as possible and in units of 2mzoe”/

mu°I”). Plot the two distributions for Q|I > 1 for nonrelativistic motion of the incident

...

(a) Calculate the cross sections for

**energy**transfer Q for close and distantcollisions (write them as functions of Q/I as far as possible and in units of 2mzoe”/

mu°I”). Plot the two distributions for Q|I > 1 for nonrelativistic motion of the incident

...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

References and suggested reading | 50 |

Copyright | |

16 other sections not shown

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