## Classical ElectrodynamicsProblems after each chapter |

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Page 211

This shows that , apart from an overall phase factor , the pulse travels along

undistorted in shape with a

an energy density is associated with the magnitude of the wave ( or its absolute ...

This shows that , apart from an overall phase factor , the pulse travels along

undistorted in shape with a

**velocity**, called the group**velocity**: do Vg ( 7.32 ) dk Ifan energy density is associated with the magnitude of the wave ( or its absolute ...

Page 331

where we have introduced a vectorial Alfvén

iwt Veikos 2 The wave equation ( 10.69 ) for v , is somewhat involved , but it

allows simple solutions for waves propagating parallel or perpendicular to the ...

where we have introduced a vectorial Alfvén

**velocity**: B. ( 10.70 ) VA = V4πρ Y -iwt Veikos 2 The wave equation ( 10.69 ) for v , is somewhat involved , but it

allows simple solutions for waves propagating parallel or perpendicular to the ...

Page 340

For wave numbers k < kp , the phase and group velocities of the longitudinal

plasma oscillations are : 0 k ( 10.107 ) 3 ( u ) V , - Up 1 From the definition of kp

we see that for such wave numbers the phase

the ...

For wave numbers k < kp , the phase and group velocities of the longitudinal

plasma oscillations are : 0 k ( 10.107 ) 3 ( u ) V , - Up 1 From the definition of kp

we see that for such wave numbers the phase

**velocity**is much larger than , andthe ...

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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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