## Classical Electrodynamics |

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Page 46

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

2.44) where a--s assantov-oso (2.45) If the interval (a, b)

of orthogonal functions U,(5) may

...

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

2.44) where a--s assantov-oso (2.45) If the interval (a, b)

**becomes**infinite, the setof orthogonal functions U,(5) may

**become**a continuum of functions, rather than a...

Page 148

55 )

proportional to the ith particle ' s orbital angular momentum , L ; = M ; ( xi x v . ) .

Thus ( 5 . 62 )

have the ...

55 )

**becomes**= 9 : ( xi x v . ) ( 5 . 62 ) 20 T The vector product ( x ; * v : ) isproportional to the ith particle ' s orbital angular momentum , L ; = M ; ( xi x v . ) .

Thus ( 5 . 62 )

**becomes**m = s _ qi L ( 5 . 63 ) 2Mic If all the particles in motionhave the ...

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

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### Contents

Introduction to Electrostatics | 1 |

References and suggested reading | 50 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

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### 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 shown in Fig shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written