## Classical ElectrodynamicsProblems after each chapter |

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Page 447

We will content ourselves with the extreme relativistic

We will content ourselves with the extreme relativistic

**limit**( B − 1 ) . ... Consequently we can approximate the Bessel functions by their small argument**limits**( 3.103 ) . Then in the relativistic**limit**the Fermi expression ( 13.70 ) ...Page 493

angles such that 0 2ka sin 2 sin 8-1 1 ( 14.112 ) If the frequency is low enough so that ka < 1 , then the

angles such that 0 2ka sin 2 sin 8-1 1 ( 14.112 ) If the frequency is low enough so that ka < 1 , then the

**limit**qa < 1 will apply at all angles . But for frequencies where ka > 1 , there will be a region of forward angles less than 1 0 ...Page 518

15.5 Radiation cross section in the complete screening

15.5 Radiation cross section in the complete screening

**limit**. The constant value is the semiclassical result . The curve marked " Bethe - Heitler " is the quantummechanical Born approximation . Wmax For extremely relativistic particles ...### What people are saying - Write a review

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

TimeVarying Fields Maxwells Equations Con | 169 |

Copyright | |

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