## Classical ElectrodynamicsProblems after each chapter |

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Page 46

a : ay0 - ( ° de ( " dnu , “ av m ( W ) ( 5,9 ) ( 2.45 ) If the interval ( a , b )

infinite , the set of orthogonal functions Un ( 5 ) may

functions , rather than a denumerable set . Then the Kronecker delta symbol in (

2.35 ) ...

a : ay0 - ( ° de ( " dnu , “ av m ( W ) ( 5,9 ) ( 2.45 ) If the interval ( a , b )

**becomes**infinite , the set of orthogonal functions Un ( 5 ) may

**become**a continuum offunctions , rather than a denumerable set . Then the Kronecker delta symbol in (

2.35 ) ...

Page 148

Then the magnetic moment ( 5.55 )

vector product ( Xi x v :) is proportional to the ith particle's orbital angular

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

particles in ...

Then the magnetic moment ( 5.55 )

**becomes**m = 2c Σφία . xv . ) ( 5.62 ) Thevector product ( Xi x v :) is proportional to the ith particle's orbital angular

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

**becomes**qi Li 2M C ( 5.63 ) If all theparticles in ...

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 | 23 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

6 other sections not shown

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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 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 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