## Classical Electrodynamics |

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Page 20

Since the Green ' s function , as a function of one of its variables , is a potential

due to a unit point charge , this symmetry merely represents the

interchangeability of the source and the observation points . For Neumann

boundary ...

Since the Green ' s function , as a function of one of its variables , is a potential

due to a unit point charge , this symmetry merely represents the

**physical**interchangeability of the source and the observation points . For Neumann

boundary ...

Page 369

6 Proper Time and the Light Cone In the previous sections we have explored

some of the

transformations . In the next two sections we want now to discuss some of the

more ...

6 Proper Time and the Light Cone In the previous sections we have explored

some of the

**physical**consequences of the special theory of relativity and Lorentztransformations . In the next two sections we want now to discuss some of the

more ...

Page 607

It depends only on the two

oscillation of the system must decay in time ( even if very slowly ) because of ever

- present resistive losses , and ( 6 ) at high frequencies binding effects are ...

It depends only on the two

**physical**requirements that ( a ) the normal modes ofoscillation of the system must decay in time ( even if very slowly ) because of ever

- present resistive losses , and ( 6 ) at high frequencies binding effects are ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

RelativisticParticle Kinematics and Dynamics | 391 |

Copyright | |

8 other sections not shown

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### Common terms and phrases

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