## 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

oscillations explicitly . These approximate

T give ...

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

**expression**, 1 1 T - 1sin 2ka + ( 9.110 ) 2ka 2,15 ( ka ) which exhibits the smalloscillations explicitly . These approximate

**expressions**( 9.109 ) and ( 9.110 ) forT give ...

Page 402

Then an explicit

1 - ( " = " " ] " 22 cos O ' ( 12.48 ) = 1 + a = Ei + m2 { [ where E ' is given by ( 12.31 )

. To obtain E , we merely interchange mz and me and change O ' into a O ...

Then an explicit

**expression**is E'2 Es = 4 € + m ) ( 1 + mo ? = min ) [ 1 - ( n + m ) ] [1 - ( " = " " ] " 22 cos O ' ( 12.48 ) = 1 + a = Ei + m2 { [ where E ' is given by ( 12.31 )

. To obtain E , we merely interchange mz and me and change O ' into a O ...

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 |

BoundaryValue Problems in Electrostatics I | 26 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

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