## Classical Electrodynamics |

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Page 402

Then an explicit

I E where E ' is given by ( 12 . 31 ) . To obtain E , we merely interchange mz and

ma and change O ' into a – O ' ( cos ' → - cos O ' ) . The relation between angles ...

Then an explicit

**expression**is * P mz – m , 2715 ( m2 + mal cos O ' ( 12 . 48 ) E 'I E where E ' is given by ( 12 . 31 ) . To obtain E , we merely interchange mz and

ma and change O ' into a – O ' ( cos ' → - cos O ' ) . The relation between angles ...

Page 446

69 ) , we find , after some calculation , the

" Reio * aK _ ( 1 * a ) K , ( ha ) - B2 ) dw ( 13 . 70 ) dx / b > a 1 v2 Jo where 2 is

given by ( 13 . 62 ) . This result can be obtained more elegantly by calculating the

...

69 ) , we find , after some calculation , the

**expression**due to Fermi , GE ) = 2 ( zey" Reio * aK _ ( 1 * a ) K , ( ha ) - B2 ) dw ( 13 . 70 ) dx / b > a 1 v2 Jo where 2 is

given by ( 13 . 62 ) . This result can be obtained more elegantly by calculating the

...

Page 447

where we have used the dipole moment

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 in the

...

where we have used the dipole moment

**expression**( 13 . 19 ) . Assuming that thesecond 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 in the

...

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### Contents

Introduction to Electrostatics | 1 |

References and suggested reading | 50 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

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