## Classical Electrodynamics |

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Page 7

However, itisoftensingler to deal with scalar rather than vector functions of

below). 1.5 Another Equation of Electrostatics and the Scalar Potential The single

equation ...

However, itisoftensingler to deal with scalar rather than vector functions of

**position**, and then to derive the vector quantities at the end if necessary (seebelow). 1.5 Another Equation of Electrostatics and the Scalar Potential The single

equation ...

Page 124

Suppose that initially the electric field E0 due to a certain distribution of charges

posk) exists in a medium of dielectric constant so which may be a function of

eoEo.

Suppose that initially the electric field E0 due to a certain distribution of charges

posk) exists in a medium of dielectric constant so which may be a function of

**position**. The initial electrostatic energy is Wo = 1 Jr. • Dodox 87 where Do =eoEo.

Page 150

In bringing the dipole m into its final

keep the current J which produces m constant. Even though the final situation is a

steady-state, there is a transient period initially in which the relevant fields are ...

In bringing the dipole m into its final

**position**in the field, work must be done tokeep the current J which produces m constant. Even though the final situation is a

steady-state, there is a transient period initially in which the relevant fields are ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

BoundaryValue Problems in Electrostatics II | 54 |

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 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 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 shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written