## Classical Electrodynamics |

### From inside the book

Results 1-3 of 85

Page 370

dr 2 1 71 1 v°(r) W - -awhere ti and to are the corresponding times in K. Another

fruitful concept in special relativity is the idea of the light cone and “

and “time-like” separations between two events. Consider Fig. 11.10, in which the

...

dr 2 1 71 1 v°(r) W - -awhere ti and to are the corresponding times in K. Another

fruitful concept in special relativity is the idea of the light cone and “

**space**-like”and “time-like” separations between two events. Consider Fig. 11.10, in which the

...

Page 371

If siz” -> 0, the events are said to have a

always possible to find a Lorentz transformation to a new coordinate system K'

where (t1' – to) = 0 and siz” = (x1' – a 2)” -- (y1' – yes)” + (21' – z,')* > 0 (11.65)

That is, ...

If siz” -> 0, the events are said to have a

**space**-like separation, because it isalways possible to find a Lorentz transformation to a new coordinate system K'

where (t1' – to) = 0 and siz” = (x1' – a 2)” -- (y1' – yes)” + (21' – z,')* > 0 (11.65)

That is, ...

Page 384

The other components of f yield similar results, showing that (11.126) can be

written as f = | F.J. k = 1,2,3 (11.128) c The right-hand side of (11.128) is evidently

the

f.

The other components of f yield similar results, showing that (11.126) can be

written as f = | F.J. k = 1,2,3 (11.128) c The right-hand side of (11.128) is evidently

the

**space**components of a 4-vector. Hence f must be the**space**part of a 4-vectorf.

### What people are saying - Write a review

#### LibraryThing Review

User Review - barriboy - LibraryThingA soul crushing technical manual written by a sadist that has served as the right of passage for physics PhDs since the dawn of time. Every single one of my professors studied this book, and every ... Read full review

#### LibraryThing Review

User Review - aproustian - LibraryThing"Jackson E&M is about learning how to approximate reliably...the entire book, with few exceptions, is a mathematical discussion on how to solve [the same] 4 problems for different boundary conditions." Read full review

### 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