## Classical Electrodynamics |

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Page 104

It should be noted that p, in general

since the distortion of the charge cloud

microscopic electric field due to the jth Fig. 4.1. A molecule with center of mass at

...

It should be noted that p, in general

**depends**on the position of x, of the molecule,since the distortion of the charge cloud

**depends**on the local field present. Themicroscopic electric field due to the jth Fig. 4.1. A molecule with center of mass at

...

Page 149

... we expect that the integral can be somehow transformed into the magnetic

moment (5.55). To accomplish this we use J x [(x'. V)B] = J x V(x'. B) = —V x [J(x' -

B)) (5.67) The first step

and ...

... we expect that the integral can be somehow transformed into the magnetic

moment (5.55). To accomplish this we use J x [(x'. V)B] = J x V(x'. B) = —V x [J(x' -

B)) (5.67) The first step

**depends**on the fact that V × B = 0 for the external field,and ...

Page 331

Then the solution for vi is a longitudinal magnetosonic wave with a phase velocity

: ulong = V s” + v 4” (10.73) Note that this wave propagates with a velocity which

...

Then the solution for vi is a longitudinal magnetosonic wave with a phase velocity

: ulong = V s” + v 4” (10.73) Note that this wave propagates with a velocity which

**depends**on the sum of hydrostatic and magnetic pressures, apart from factors of...

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### Contents

Introduction to Electrostatics | 1 |

Nē 3 | 3 |

Greens theorem | 14 |

Copyright | |

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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge classical collisions compared component conducting conductor Consequently consider constant coordinates cross section cylinder defined density depends 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 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 result satisfy scalar scattering shows side simple solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written