## Classical Electrodynamics |

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Page 310

called plasma

low ...

**Oscillations**occur in the charge density . These high - frequency**oscillations**arecalled plasma

**oscillations**and are to be distinguished from lower - frequency**oscillations**which involve motion of the fluid , but no charge separation . Theselow ...

Page 341

108 ) shows that for k < kp the longitudinal plasma

undamped . But the damping becomes important as soon as k ~ kp ( even for k =

0 . 5kD , Im 0 - - 0 . 70p ) . For wave numbers larger than the Debye wave number

the ...

108 ) shows that for k < kp the longitudinal plasma

**oscillations**are virtuallyundamped . But the damping becomes important as soon as k ~ kp ( even for k =

0 . 5kD , Im 0 - - 0 . 70p ) . For wave numbers larger than the Debye wave number

the ...

Page 628

Cylindrical coordinates, Laplace's equation in, 69 separation of variables in, 69

waves in, 241 Damping, of magnetohydrodynamic waves, 333 of

cavity, 255 of plasma

Cylindrical coordinates, Laplace's equation in, 69 separation of variables in, 69

waves in, 241 Damping, of magnetohydrodynamic waves, 333 of

**oscillations**incavity, 255 of plasma

**oscillations**, 340 see also Radiative reaction Darwin-Breit ...### What people are saying - Write a review

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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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### 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