## Classical ElectrodynamicsProblems after each chapter |

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Page 46

( 2.45 ) If the interval ( a , b )

( 2.45 ) If the interval ( a , b )

**becomes**infinite , the set of orthogonal functions Uņ ( 5 ) may**become**a continuum of functions , rather than a ...Page 148

Then the magnetic moment ( 5.55 )

Then the magnetic moment ( 5.55 )

**becomes**1 9. ( Xi X v :) ( 5.62 ) 2c m = Σακα , και i The vector product ( xi x v :) is proportional to the ith particle's ...Page 310

Then inertial effects enter and the conductivity

Then inertial effects enter and the conductivity

**becomes**complex . Unfortunately at these same frequencies the description of collisions in terms of a ...### What people are saying - Write a review

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### Contents

Introduction to Electrostatics | 1 |

Greens theorem | 14 |

BoundaryValue Problems in Electrostatics I | 26 |

Copyright | |

9 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 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 sphere spherical surface transformation unit vanishes vector velocity volume wave written