## Classical Electrodynamics |

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Page 25

Show that the capacitance per unit length is

In - where a is the geometrical mean of the two radii . Approximately what B & S

gauge wire ( state diameter in millimeters as well as gauge ) would be necessary

...

Show that the capacitance per unit length is

**given**approximately by C ~ ( 41n 14In - where a is the geometrical mean of the two radii . Approximately what B & S

gauge wire ( state diameter in millimeters as well as gauge ) would be necessary

...

Page 229

For propagation in directions other than parallel to the static field B , it is

straightforward to show that , if terms of the order of wb ? are neglected compared

to wè and wwb , the index of refraction is still

precession ...

For propagation in directions other than parallel to the static field B , it is

straightforward to show that , if terms of the order of wb ? are neglected compared

to wè and wwb , the index of refraction is still

**given**by ( 7 . 102 ) . But theprecession ...

Page 305

More complete discussions of antennas and antenna arrays are

engineering works , such as Jordan , Kraus , Schelkunoff , Silver . The subject of

diffraction has a very extensive literature . A comprehensive treatment of both the

scalar ...

More complete discussions of antennas and antenna arrays are

**given**inengineering works , such as Jordan , Kraus , Schelkunoff , Silver . The subject of

diffraction has a very extensive literature . A comprehensive treatment of both the

scalar ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

RelativisticParticle Kinematics and Dynamics | 391 |

Copyright | |

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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge charged particle classical collisions compared component conducting Consequently consider constant coordinates cross section cylinder defined density dependence derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved light limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means modes momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative relativistic result satisfy scalar scattering shown in Fig shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written