## Classical ElectrodynamicsProblems after each chapter |

### From inside the book

Results 1-3 of 70

Page 181

6.5 Gauge Transformations ;

transformation ( 6.34 ) and ( 6.35 ) is called a gauge transformation , and the

invariance of the fields under such transformations is called gauge invariance .

The relation ( 6.36 ) ...

6.5 Gauge Transformations ;

**Lorentz**Gauge ; Coulomb Gauge Thetransformation ( 6.34 ) and ( 6.35 ) is called a gauge transformation , and the

invariance of the fields under such transformations is called gauge invariance .

The relation ( 6.36 ) ...

Page 367

At time t the electron's rest frame K'and the laboratory frame K are related by a

now changed to K " , related to K by a

At time t the electron's rest frame K'and the laboratory frame K are related by a

**Lorentz**transformation with velocity v . At time 1 + dt the electron's rest frame hasnow changed to K " , related to K by a

**Lorentz**transformation with velocity v + dv .Page

Ives - Stilwell experiment , 364 Jacobian , in

coordinates , 376 in transforming delta functions , 79 Kinematics , relativistic , 394

f . Kirchhoff diffraction , see Diffraction Kirchhoff's integral representation , 188

use of , in ...

Ives - Stilwell experiment , 364 Jacobian , in

**Lorentz**transformation ofcoordinates , 376 in transforming delta functions , 79 Kinematics , relativistic , 394

f . Kirchhoff diffraction , see Diffraction Kirchhoff's integral representation , 188

use of , in ...

### 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 |

Greens theorem | 14 |

BoundaryValue Problems in Electrostatics I | 26 |

Copyright | |

9 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 limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means 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 sphere spherical surface transformation unit vanishes vector velocity volume wave written