## Classical ElectrodynamicsProblems after each chapter |

### From inside the book

Results 1-3 of 71

Page 412

The

uniform translation parallel to B. The solution for the velocity is easily shown to be

v(0 = vfo + roaafo - ieje-***' (12.95) where e3 is a unit vector parallel to the field, ...

The

**motion**described by (12.93) is a circular**motion**perpendicular to B and auniform translation parallel to B. The solution for the velocity is easily shown to be

v(0 = vfo + roaafo - ieje-***' (12.95) where e3 is a unit vector parallel to the field, ...

Page 501

14.5 As in Problem 14.2a a charge e moves in simple harmonic

z axis, z(t') = a cos (eo0/'). (a) Show that the instantaneous power radiated per

unit solid angle is: dP(t') ^ e2cp sin2 6 cos2 (eop rfQ " 4«z2 (1 + p cos 6 sin ay')5 ...

14.5 As in Problem 14.2a a charge e moves in simple harmonic

**motion**along thez axis, z(t') = a cos (eo0/'). (a) Show that the instantaneous power radiated per

unit solid angle is: dP(t') ^ e2cp sin2 6 cos2 (eop rfQ " 4«z2 (1 + p cos 6 sin ay')5 ...

Page 578

Antennas and radiation from multipole sources are examples of the first type of

problem, while

phenomena are examples of the second type. Occasionally, as in the discussion

...

Antennas and radiation from multipole sources are examples of the first type of

problem, while

**motion**of charges in electric and magnetic fields and energy-lossphenomena are examples of the second type. Occasionally, as in the discussion

...

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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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### Common terms and phrases

acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge charged particle classical coefficients 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 shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written