## Classical ElectrodynamicsProblems after each chapter |

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Page 10

To find the potential due to a

then superpose a surface density of them , or we can obtain the same result by

performing mathematically the limiting process described in words above on the

...

To find the potential due to a

**dipole**layer we can consider a single**dipole**andthen superpose a surface density of them , or we can obtain the same result by

performing mathematically the limiting process described in words above on the

...

Page 132

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

. In the presence of magnetic materials the

direction . That direction is by definition the direction of the magnetic - flux ...

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 certaindirection . That direction is by definition the direction of the magnetic - flux ...

Page 274

Considering only the magnetization term , we have the vector potential , iker 1 A (

x ) ik ( n x m ) ) ( 9.33 ) ikr where m is the magnetic

že Sex * J ) des ( 9.34 ) The fields can be determined by noting that the vector ...

Considering only the magnetization term , we have the vector potential , iker 1 A (

x ) ik ( n x m ) ) ( 9.33 ) ikr where m is the magnetic

**dipole**moment , m = -fmær -že Sex * J ) des ( 9.34 ) The fields can be determined by noting that the vector ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Wave Guides and Resonant Cavities | 235 |

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