## Classical Electrodynamics |

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Page 233

( c )

coefficient is 32 ( Re ) % e – 21 / 8 1 - 2e - 21 / 8 cos ( 2t / 8 ) + e - 4t / 8 Sketch log

T as a function of ( t | 8 ) , assuming Re B = 10 - 2 . Define “ very small thickness .

” 7 .

( c )

**Show**that , except for sheets of very small thickness , the transmissioncoefficient is 32 ( Re ) % e – 21 / 8 1 - 2e - 21 / 8 cos ( 2t / 8 ) + e - 4t / 8 Sketch log

T as a function of ( t | 8 ) , assuming Re B = 10 - 2 . Define “ very small thickness .

” 7 .

Page 365

The Thomas precession , as it is called , also gives a qualitative explanation for a

spinorbit interaction in atomic nuclei and

in nuclei . The Uhlenbeck - Goudsmit hypothesis was that an electron ...

The Thomas precession , as it is called , also gives a qualitative explanation for a

spinorbit interaction in atomic nuclei and

**shows**why the doublets are “ inverted ”in nuclei . The Uhlenbeck - Goudsmit hypothesis was that an electron ...

Page 367

21 ) twice , it is a straightforward matter to

K ' are related by t " = t X ( 11 . ... This

to K " involves an infinitesimal Lorentz transformation with a velocity lv . dy 7 ...

21 ) twice , it is a straightforward matter to

**show**that the time variables in K " andK ' are related by t " = t X ( 11 . ... This

**shows**that the direct transformation from K 'to K " involves an infinitesimal Lorentz transformation with a velocity lv . dy 7 ...

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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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