## Classical ElectrodynamicsProblems after each chapter |

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Page 295

For ka > 1 , the second form in ( 9.109 ) can be used to obtain an asymptotic

For ka > 1 , the second form in ( 9.109 ) can be used to obtain an asymptotic

**expression**, 1 1 TT T - 1sin ( 2ka 2,15 ( ka ) + ( 9.110 ) 2ka 4 which exhibits the small oscillations explicitly . These approximate**expressions**( 9.109 ) ...Page 446

The Fermi

The Fermi

**expression**( 13.70 ) bears little resemblance to our previous results for energy loss , such as ( 13.35 ) . But under conditions where polarization effects are unimportant it yields the same results as before .Page 447

where we have used the dipole moment

where we have used the dipole moment

**expression**( 13.19 ) . Assuming that the second term is small , the imaginary part of 1 / € ( w ) can be readily calculated and substituted into ( 13.70 ) . Then the integral over do can be performed ...### 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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