## Classical ElectrodynamicsProblems after each chapter |

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Page 10

The

The

**dipole**- layer distribution of strength D ( x ) is formed by letting S ' approach infinitesimally close to S while the surface - charge density o ( x ) becomes infinite in such a manner that the product of g ...Page 132

The basic entity in magnetic studies was what we now know as a magnetic

The basic entity in magnetic studies was what we now know as a magnetic

**dipole**. In the presence of magnetic materials the**dipole**tends to align itself in a certain direction . That direction is by definition the direction of the ...Page 274

Considering only the magnetization term , we have the vector potential , eikr A ( x ) = ik ( n x m ) ( 9.33 ) r ikr where m is the magnetic

Considering only the magnetization term , we have the vector potential , eikr A ( x ) = ik ( n x m ) ( 9.33 ) r ikr where m is the magnetic

**dipole**moment , m = = -1 & r = [ x sixx J ) ( 9.34 ) The fields can be determined by noting that ...### 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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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