## Classical ElectrodynamicsProblems after each chapter |

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Page 18

In obtaining result ( 1.36 ) —not a solution — we chose the function y to be 1 / 1X – X ' ] , it being the potential of a unit point charge ,

In obtaining result ( 1.36 ) —not a solution — we chose the function y to be 1 / 1X – X ' ] , it being the potential of a unit point charge ,

**satisfying**the ...Page 181

To see that potentials can always be found to

To see that potentials can always be found to

**satisfy**the Lorentz condition , suppose that the potentials A , 0 which**satisfy**( 6.32 ) and ( 6.33 ) do not ...Page 287

... Of course , the fields E ' , B ' must

... Of course , the fields E ' , B ' must

**satisfy**Maxwell's equations and the radiation condition in region II ' if E , B**satisfy**them in region II .### What people are saying - Write a review

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User Review - aproustian - LibraryThing"Jackson E&M is about learning how to approximate reliably...the entire book, with few exceptions, is a mathematical discussion on how to solve [the same] 4 problems for different boundary conditions." Read full review

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