## Classical Electrodynamics |

### From inside the book

Results 1-3 of 75

Page 63

John David Jackson. If the point x is on the z

to ( 3 . 38 ) , while the left - hand side becomes : ( 3 : 43 ) ( 3 . 43 ) X – x ' ( p2 + p 2

– 2rr ' cos y ) " ir – pl Expanding ( 3 . 43 ) , we find x + 21 + 2 + y2 – 2mp cos y ' i ...

John David Jackson. If the point x is on the z

**axis**, the right - hand side reducesto ( 3 . 38 ) , while the left - hand side becomes : ( 3 : 43 ) ( 3 . 43 ) X – x ' ( p2 + p 2

– 2rr ' cos y ) " ir – pl Expanding ( 3 . 43 ) , we find x + 21 + 2 + y2 – 2mp cos y ' i ...

Page 166

( c ) Show that at the end of a long solenoid the magnetic induction near the

has components B . < 20NI , B , " NI ( 9 ) 5 . 3 A cylindrical conductor of radius a

has a hole of radius b bored parallel to , and centered a distance d from , the ...

( c ) Show that at the end of a long solenoid the magnetic induction near the

**axis**has components B . < 20NI , B , " NI ( 9 ) 5 . 3 A cylindrical conductor of radius a

has a hole of radius b bored parallel to , and centered a distance d from , the ...

Page 422

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

0 , 2 = vo ? ( 12 . 126 ) where vol = 0 . 102 + 0 . 102 is the square of the speed at

z = 0 . If we assume that the flux linked is a constant of the motion , then ( 12 .

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

**axis**0 , 2 +0 , 2 = vo ? ( 12 . 126 ) where vol = 0 . 102 + 0 . 102 is the square of the speed at

z = 0 . If we assume that the flux linked is a constant of the motion , then ( 12 .

### 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