## Classical Electrodynamics |

### From inside the book

Results 1-3 of 64

Page 7

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

below ) . 1 . 5 Another Equation of Electrostatics and the Scalar Potential The

single ...

However , itis often simpler 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 ...

Page 124

... constant e , which may be a function of

is Wo = JE • Do doc 8TT where Do = 6 En . Then with the sources fixed in

a dielectric object of volume V , is introduced into the field , changing the field ...

... constant e , which may be a function of

**position**. The initial electrostatic energyis Wo = JE • Do doc 8TT where Do = 6 En . Then with the sources fixed in

**position**a dielectric object of volume V , is introduced into the field , changing the field ...

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

...

### What people are saying - Write a review

We haven't found any reviews in the usual places.

### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

RelativisticParticle Kinematics and Dynamics | 391 |

Copyright | |

8 other sections not shown

### Other editions - View all

### 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