## Classical Electrodynamics |

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Make a sketch of I as a function of X for fixed Z. (c) Use the vector formula (9.82)

to obtain a

linearly polarized plane wave of amplitude Eo and wave number k is incident on

a ...

Make a sketch of I as a function of X for fixed Z. (c) Use the vector formula (9.82)

to obtain a

**result**equivalent to that of part (a). Compare the two expressions. Alinearly polarized plane wave of amplitude Eo and wave number k is incident on

a ...

Page

John David Jackson. below which our approximate

replaced by a more exact expression which tends to (13.5) as b → 0. It can be

shown (Problem 13.1) that a proper treatment gives the more accurate

John David Jackson. below which our approximate

**result**(13.2) must bereplaced by a more exact expression which tends to (13.5) as b → 0. It can be

shown (Problem 13.1) that a proper treatment gives the more accurate

**result**, ...Page

14.3, then the power radiated can be written *~ _dP e” - + = — to sin” (9 - 14.21 d

() 4trc” ( ) This exhibits the characteristic sin” (9 angular dependence which is a

wellknown

...

14.3, then the power radiated can be written *~ _dP e” - + = — to sin” (9 - 14.21 d

() 4trc” ( ) This exhibits the characteristic sin” (9 angular dependence which is a

wellknown

**result**. We note from (14.18) that the radiation is polarized in the plane...

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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 sphere spherical surface transformation unit vanishes vector velocity volume wave written