## Classical Electrodynamics |

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Page 472

For relativistic motion the

14.14) the radial component of Poynting's vector can be calculated to be |n x [(n ...

For relativistic motion the

**acceleration**fields depend on the velocity as well as the**acceleration**. Consequently the angular distribution is more complicated. From (14.14) the radial component of Poynting's vector can be calculated to be |n x [(n ...

Page 475

The total power radiated can be found by integrating (14.44) over all angles or

from (14.26): 2.2 P(t) = **:::/ (14.46) 3 co It is instructive to compare the power

radiated for

...

The total power radiated can be found by integrating (14.44) over all angles or

from (14.26): 2.2 P(t) = **:::/ (14.46) 3 co It is instructive to compare the power

radiated for

**acceleration**parallel to the velocity (14.43) or (14.27) with the power...

Page 506

The sudden creation of a fast electron in nuclear beta decay, for example, can be

viewed for our purposes as the violent

at rest to some final velocity in a very short time interval, or, alternatively, as the ...

The sudden creation of a fast electron in nuclear beta decay, for example, can be

viewed for our purposes as the violent

**acceleration**of a charged particle initiallyat rest to some final velocity in a very short time interval, or, alternatively, as the ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

5 other sections not shown

### 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 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