## Classical Electrodynamics |

### From inside the book

Results 1-3 of 84

Page 46

Then the expansion of an arbitrary function f(&, m) is f(#, n) = 2, 2 a.m.U.($)W.(m)

(2.44) where b d 0nm –s d;s dm U,"(3)W,"(m)f($, m) (2.45) If the interval (a, b)

of ...

Then the expansion of an arbitrary function f(&, m) is f(#, n) = 2, 2 a.m.U.($)W.(m)

(2.44) where b d 0nm –s d;s dm U,"(3)W,"(m)f($, m) (2.45) If the interval (a, b)

**becomes**infinite, the set of orthogonal functions U,($) may**become**a continuumof ...

Page 148

Then the magnetic moment (5.55)

product (x, x v.) is proportional to the ith particle's orbital angular momentum, Li =

M.(x, x v.). Thus (5.62)

have ...

Then the magnetic moment (5.55)

**becomes**m = #26. x vi) (5.62) The vectorproduct (x, x v.) is proportional to the ith particle's orbital angular momentum, Li =

M.(x, x v.). Thus (5.62)

**becomes**- qi in -2Mc Li (5.63) If all the particles in motionhave ...

Page 310

Then inertial effects enter and the conductivity

at these same frequencies the description of collisions in terms of a frictional

force tends to lose its validity. The whole process

Then inertial effects enter and the conductivity

**becomes**complex. Unfortunatelyat these same frequencies the description of collisions in terms of a frictional

force tends to lose its validity. The whole process

**becomes**more complicated.### 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