## Classical Electrodynamics |

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Page 52

... on the surface of a

halves of a long conducting

and ...

... on the surface of a

**cylinder**of radius b, and show that the solution inside the**cylinder**is given by Poisson's integral: b? — r? b” + r* – 2br cos (9 – 6) (b) Twohalves of a long conducting

**cylinder**of radius b are separated by a small gap,and ...

Page 95

A hollow right circular

and its ends at z = 0 and z = L. The potential on the end faces is zero, while the

potential on the cylindrical surface is given as V(4,2). Using the appropriate ...

A hollow right circular

**cylinder**of radius b has its axis coincident with the z axisand its ends at z = 0 and z = L. The potential on the end faces is zero, while the

potential on the cylindrical surface is given as V(4,2). Using the appropriate ...

Page 260

The axial propagation constant k must be the same inside and outside the

times. In the usual way, inside the dielectric

the ...

The axial propagation constant k must be the same inside and outside the

**cylinder**in order to satisfy boundary conditions at all points on the surface at alltimes. In the usual way, inside the dielectric

**cylinder**the transverse Laplacian ofthe ...

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### Contents

Introduction to Electrostatics | 1 |

References and suggested reading | 23 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

6 other sections not shown

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