## Classical Electrodynamics |

### From inside the book

Results 1-3 of 88

Page 237

First we

field E , and a tangential magnetic field H . , , as for a perfect conductor . The

values of these fields are

...

First we

**assume**that just outside the conductor there exists only a normal electricfield E , and a tangential magnetic field H . , , as for a perfect conductor . The

values of these fields are

**assumed**to have been obtained from the solution of an...

Page 241

For simplicity , the cross - sectional size and shape are

the cylinder axis . With a sinusoidal time dependence e - iwt for the fields inside

the cylinder , Maxwell ' s equations take the form : V E = i B D . B = 0 ( 8 . 16 ) V x

...

For simplicity , the cross - sectional size and shape are

**assumed**constant alongthe cylinder axis . With a sinusoidal time dependence e - iwt for the fields inside

the cylinder , Maxwell ' s equations take the form : V E = i B D . B = 0 ( 8 . 16 ) V x

...

Page 297

The dimensions of the hole are

wavelength of the electromagnetic fields which are

of the sheet . The problem is to calculate the diffracted fields on the other side of

the ...

The dimensions of the hole are

**assumed**to be very small compared to awavelength of the electromagnetic fields which are

**assumed**to exist on one sideof the sheet . The problem is to calculate the diffracted fields on the other side of

the ...

### 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