## Classical ElectrodynamicsProblems after each chapter |

### From inside the book

Results 1-3 of 78

Page 233

( C )

coefficient is 32 ( Re B ) e - 21 / 0 T 1 – 2e - 2t / 8 cos ( 21/8 ) + e - 4t / 8 Sketch log

T as a function of ( t / 8 ) , assuming Re B = 10-2 . Define “ very small thickness .

( C )

**Show**that , except for sheets of very small thickness , the transmissioncoefficient is 32 ( Re B ) e - 21 / 0 T 1 – 2e - 2t / 8 cos ( 21/8 ) + e - 4t / 8 Sketch log

T as a function of ( t / 8 ) , assuming Re B = 10-2 . Define “ very small thickness .

Page 369

From ( 11.21 ) it is easy to

dz2 c2 dt2 ( 11.61 ) In terms of the particle velocity v ( t ) this can be written dr = dt

ati( 11.62 ) Equation ( 11.62 )

.

From ( 11.21 ) it is easy to

**show**that the invariant “ length " element is ds ? ... +dz2 c2 dt2 ( 11.61 ) In terms of the particle velocity v ( t ) this can be written dr = dt

ati( 11.62 ) Equation ( 11.62 )

**shows**the time - dilatation effect already discussed.

Page 501

( a )

e cp4 sina 0 cos ( wt ) d22 4ma ? ( 1 + B cos sin wot ' ) where B = 20 / c . ( b ) By

performing a time averaging ,

...

( a )

**Show**that the instantaneous power radiated per unit solid angle is : dP ( t ' )e cp4 sina 0 cos ( wt ) d22 4ma ? ( 1 + B cos sin wot ' ) where B = 20 / c . ( b ) By

performing a time averaging ,

**show**that the average power per unit solid angle is...

### 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 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

4 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 coefficients 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 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