## Classical ElectrodynamicsProblems after each chapter |

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Page 359

If it lives a time t , in K ' , then at its instant of decay , we find t z c2 t ' = To = ( 11.23

) v2 c2 1 То T = The time t is the meson's lifetime 7 as observed in the system K.

...

If it lives a time t , in K ' , then at its instant of decay , we find t z c2 t ' = To = ( 11.23

) v2 c2 1 То T = The time t is the meson's lifetime 7 as observed in the system K.

**Consequently**( 11.24 ) 1 ca When viewed from K the moving meson lives longer...

Page 447

limits ( 3.103 ) . Then in the relativistic limit the Fermi expression ( 13.70 ) is de 2 (

ze ) Re ιω dx / b > a le ( w ) 1.123c In In ( 1 2 It is worth while right here to point ...

**Consequently**we can approximate the Bessel functions by their small argumentlimits ( 3.103 ) . Then in the relativistic limit the Fermi expression ( 13.70 ) is de 2 (

ze ) Re ιω dx / b > a le ( w ) 1.123c In In ( 1 2 It is worth while right here to point ...

Page 508

of the radiation is a natural one with respect to which one specifies the state of

polarization of the radiation . For simplicity we consider a small angle deflection

so ...

**Consequently**the plane containing the incident beam direction and the directionof the radiation is a natural one with respect to which one specifies the state of

polarization of the radiation . For simplicity we consider a small angle deflection

so ...

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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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