## Classical Electrodynamics |

### From inside the book

Results 1-3 of 75

Page 63

If the point x is on the z

hand side becomes: 1 — 1 1 |x – x' T (r” + r.” – 2rr'cos y)* ' |r – r" (3.43) Expanding

(3.43), we find H = + > (#) (3.44) For points off the

If the point x is on the z

**axis**, the right-hand side reduces to (3.38), while the left-hand side becomes: 1 — 1 1 |x – x' T (r” + r.” – 2rr'cos y)* ' |r – r" (3.43) Expanding

(3.43), we find H = + > (#) (3.44) For points off the

**axis**it is only necessary, ...Page 166

c c \ a A cylindrical conductor of radius a has a hole of radius b bored parallel to,

and centered a distance d from, the cylinder

uniform throughout the remaining metal of the cylinder and is parallel to the

c c \ a A cylindrical conductor of radius a has a hole of radius b bored parallel to,

and centered a distance d from, the cylinder

**axis**(d + b : a). The current density isuniform throughout the remaining metal of the cylinder and is parallel to the

**axis**...Page 422

The speed of the particle is constant so that at any position along the z

.” = to (12.126) where to - vu" + vo” is the square of the speed at z = 0. If we

assume that the flux linked is a constant of the motion, then (12.125) allows us to

write ...

The speed of the particle is constant so that at any position along the z

**axis**vo + v.” = to (12.126) where to - vu" + vo” is the square of the speed at z = 0. If we

assume that the flux linked is a constant of the motion, then (12.125) allows us to

write ...

### 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 |

BoundaryValue Problems in Electrostatics II | 54 |

Copyright | |

16 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 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