## 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**, T T - 1 1 2ka 1 sin 2ka 21 ( ka ) + . ( 9.110 ) 4 . which exhibits the small oscillations explicitly . These approximate**expressions**( 9.109 ) ...Page 402

Then an explicit

Then an explicit

**expression**is m ) Ez = { ( E + m2 ) 1 + E'2 + } { [ 4- ( " , # m . ) } ] [ - ( , moji ] " cos O ' ( 12.48 ) tan 03 q'sin O ' tan 02 1+ a = { where E ' is given by ( 12.31 ) . To obtain Eq we merely interchange mz and me ...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 / € ( 0 ) 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 |

References and suggested reading | 23 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

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