## Classical ElectrodynamicsProblems after each chapter |

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Page 7

However , it is often simpler to deal with scalar rather than vector functions of

However , it is often simpler to deal with scalar rather than vector functions of

**position**, and then to derive the vector quantities at the end if necessary ( see below ) . Another Equation of Electrostatics and the Scalar Potential ...Page 124

Suppose that initially the electric field E , due to a certain distribution of charges po ( x ) exists in a medium of dielectric constant E , which may be a function of

Suppose that initially the electric field E , due to a certain distribution of charges po ( x ) exists in a medium of dielectric constant E , which may be a function of

**position**. The initial electrostatic energy is Wo o se , D. , dr ...Page 150

In bringing the dipole m into its final

In bringing the dipole m into its final

**position**in the field , work must be done to 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 ...### What people are saying - Write a review

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

TimeVarying Fields Maxwells Equations Con | 169 |

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