## Classical Electrodynamics |

### From inside the book

Results 1-3 of 79

Page 46

Then the expansion of an arbitrary function f($, m) is f(k, n) = 2, 2 a.m.U.(5)W,(m) (

2.44) where b d sk + ann = | d5 | dou,"($)V,"(m)f($, m) (2.45) If the interval (a, b)

Then the expansion of an arbitrary function f($, m) is f(k, n) = 2, 2 a.m.U.(5)W,(m) (

2.44) where b d sk + ann = | d5 | dou,"($)V,"(m)f($, m) (2.45) If the interval (a, b)

**becomes**infinite, the set of orthogonal functions U,($) may**become**a continuum ...Page 148

... position of the ith particle. Then the magnetic moment (5.55)

X*. x vi) (5.62) The vector product (x, x v.) is proportional to the ith particle's orbital

angular momentum, L = M.(x, x v.). Thus (5.62)

... position of the ith particle. Then the magnetic moment (5.55)

**becomes**1 in E. #X*. x vi) (5.62) The vector product (x, x v.) is proportional to the ith particle's orbital

angular momentum, L = M.(x, x v.). Thus (5.62)

**becomes**qi m = X —#1– L 5.63 ...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

We haven't found any reviews in the usual places.

### Contents

Introduction to Electrostatics | 1 |

Nš 3 | 3 |

Greens theorem | 14 |

Copyright | |

30 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 conductor Consequently consider constant coordinates cross section cylinder defined density depends 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 result satisfy scalar scattering shows side simple solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written