## Classical ElectrodynamicsProblems after each chapter |

### From inside the book

Results 1-3 of 53

Page 251

Thus , using ( 8.59 ) with ( 8.62 ) and ( 8.51 ) , plus the frequency

the skin depth ( 7.85 ) , we find ( 3 ) 1 С - Calle fi ☺ 471 N. 2A ξ Eitni 101 ] ( 8.63 )

* 02 where o is ihe conductivity ( assumed independent of frequency ) , 8 , is the ...

Thus , using ( 8.59 ) with ( 8.62 ) and ( 8.51 ) , plus the frequency

**dependence**ofthe skin depth ( 7.85 ) , we find ( 3 ) 1 С - Calle fi ☺ 471 N. 2A ξ Eitni 101 ] ( 8.63 )

* 02 where o is ihe conductivity ( assumed independent of frequency ) , 8 , is the ...

Page 269

John David Jackson, Patrick Thaddeus Jackson. As usual , the real part of such

expressions is to be taken to obtain physical quantities . The electromagnetic

potentials and fields are assumed to have the same time

shown ...

John David Jackson, Patrick Thaddeus Jackson. As usual , the real part of such

expressions is to be taken to obtain physical quantities . The electromagnetic

potentials and fields are assumed to have the same time

**dependence**. It wasshown ...

Page 296

Both formulas contain the same “ diffraction " distribution factor [ J / ( ka5 ) / kat ]

and the same

azimuthal

expression ...

Both formulas contain the same “ diffraction " distribution factor [ J / ( ka5 ) / kat ]

and the same

**dependence**on wave number . But the scalar result has noazimuthal

**dependence**( apart from that contained in ) , whereas the vectorexpression ...

### 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