## Classical Electrodynamics |

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Page 193

93 ) transform like

divergence of some quantity , that quantity must be a tensor of the second rank .

While it is possible to deal with rectangular components of momentum , instead of

...

93 ) transform like

**vectors**. Consequently , if they are to be combined into thedivergence of some quantity , that quantity must be a tensor of the second rank .

While it is possible to deal with rectangular components of momentum , instead of

...

Page 307

Make a sketch of I as a function of X for fixed Z . ( c ) Use the

82 ) to obtain a result equivalent to that of part ( a ) . Compare the two

expressions . A linearly polarized plane wave of amplitude E , and wave number

k is incident ...

Make a sketch of I as a function of X for fixed Z . ( c ) Use the

**vector**formula ( 9 .82 ) to obtain a result equivalent to that of part ( a ) . Compare the two

expressions . A linearly polarized plane wave of amplitude E , and wave number

k is incident ...

Page 640

cartesian coordinates, 141 of localized oscillating source, 269 f. of magnetic

dipole, 146 of oscillating electric dipole, 271 of oscillating electric quadrupole,

275 of ...

**Vector**potential, for time-varying fields, 179 in magnetostatics, 139 f. in non-cartesian coordinates, 141 of localized oscillating source, 269 f. of magnetic

dipole, 146 of oscillating electric dipole, 271 of oscillating electric quadrupole,

275 of ...

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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