## Classical ElectrodynamicsProblems after each chapter |

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Page 269

John David Jackson, Patrick Thaddeus Jackson. As usual , the real part of such

expressions is to be taken to obtain physical quantities . The electromagnetic

potentials and fields are assumed to have the same time

shown ...

John David Jackson, Patrick Thaddeus Jackson. As usual , the real part of such

expressions is to be taken to obtain physical quantities . The electromagnetic

potentials and fields are assumed to have the same time

**dependence**. It wasshown ...

Page 296

Both formulas contain the same " diffraction " distribution factor [ J / ( kaş ) / kat ] ?

and the same

azimuthal

Both formulas contain the same " diffraction " distribution factor [ J / ( kaş ) / kat ] ?

and the same

**dependence**on wave number . But the scalar result has noazimuthal

**dependence**( apart from that contained in 5 ) , whereas the vector ...Page 553

Furthermore , we assume that the time

Fourier components , and we consider only harmonically varying sources , p ( x )

e - iwt , J ( x ) e - iet M ( x ) e - int ( 16.76 ) where it is understood that we take the

real ...

Furthermore , we assume that the time

**dependence**can be analyzed into itsFourier components , and we consider only harmonically varying sources , p ( x )

e - iwt , J ( x ) e - iet M ( x ) e - int ( 16.76 ) where it is understood that we take the

real ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

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