## Classical ElectrodynamicsProblems after each chapter |

### From inside the book

Results 1-3 of 81

Page 233

( c )

coefficient is 32 ( Re B ) e - 2018 T 1 cos ( 2t / 8 ) + e - 4t / 8 Sketch log T as a

function of ( t / 8 ) , assuming Re ß = 10-2 Define “ very small thickness . ” 7.6

Plane waves ...

( c )

**Show**that , except for sheets of very small thickness , the transmissioncoefficient is 32 ( Re B ) e - 2018 T 1 cos ( 2t / 8 ) + e - 4t / 8 Sketch log T as a

function of ( t / 8 ) , assuming Re ß = 10-2 Define “ very small thickness . ” 7.6

Plane waves ...

Page 365

Equation ( 11.39 )

electron moves ... We will

moving with the electron the magnetic induction is B ' - B x E ( 11.41 ) с where we

have ...

Equation ( 11.39 )

**shows**that the electron has a g factor of 2. Suppose that anelectron moves ... We will

**show**in Section 11.10 that in a coordinate systemmoving with the electron the magnetic induction is B ' - B x E ( 11.41 ) с where we

have ...

Page 367

Using the general formula ( 11.21 ) twice , it is a straightforward matter to

that the time variables in K " and K ' are related by 1 V. δν t " = t - 1 ( 11.50 ) v2 v2

1 c2 correct to first order in dv . This

to ...

Using the general formula ( 11.21 ) twice , it is a straightforward matter to

**show**that the time variables in K " and K ' are related by 1 V. δν t " = t - 1 ( 11.50 ) v2 v2

1 c2 correct to first order in dv . This

**shows**that the direct transformation from K 'to ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Wave Guides and Resonant Cavities | 235 |

Copyright | |

5 other sections not shown

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