## Classical ElectrodynamicsProblems after each chapter |

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Page 99

Equation ( 4.1 ) is

Equation ( 4.1 ) is

**called**a multipole expansion ; the 1 = 0 term is**called**the monopole term , 1 = 1 is the dipole term , etc. The reason for these names ...Page 140

If V.B = 0 everywhere , B must be the curl of some vector field A ( x ) ,

If V.B = 0 everywhere , B must be the curl of some vector field A ( x ) ,

**called**the vector potential , B ( x ) = V X A ( x ) ( 5.27 ) We have , in fact ...Page 181

6.5 Gauge Transformations ; Lorentz Gauge ; Coulomb Gauge The transformation ( 6.34 ) and ( 6.35 ) is

6.5 Gauge Transformations ; Lorentz Gauge ; Coulomb Gauge The transformation ( 6.34 ) and ( 6.35 ) is

**called**a gauge transformation , and the invariance of ...### 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 | |

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