## Classical Electrodynamics |

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Page 233

(c)

coefficient is 32(Rep)?e-Atlo 1 – 2e-*locos (21/6) + e-419 Sketch log T as a

function of (t|6), assuming Re B = 10−". Define “very small thickness.” 7.6 Plane

waves ...

(c)

**Show**that, except for sheets of very small thickness, the transmissioncoefficient is 32(Rep)?e-Atlo 1 – 2e-*locos (21/6) + e-419 Sketch log T as a

function of (t|6), assuming Re B = 10−". Define “very small thickness.” 7.6 Plane

waves ...

Page 369

From (11.21) it is easy to

+ dz” – c' dt” (11.60) This leads ... particle velocity v(t) this can be written U2 *-*.si

To (11.62) Equation (11.62)

From (11.21) it is easy to

**show**that the invariant “length” element is ds” = dr” + dy”+ dz” – c' dt” (11.60) This leads ... particle velocity v(t) this can be written U2 *-*.si

To (11.62) Equation (11.62)

**shows**the time-dilatation effect already discussed.Page 501

(a)

" sin” 0 cos” (ot') d.T T.47 (TTB coso sin of); where 3 = awolc. (b) By performing a

time averaging,

(a)

**Show**that the instantaneous power radiated per unit solid angle is: dP(t) e°cB" sin” 0 cos” (ot') d.T T.47 (TTB coso sin of); where 3 = awolc. (b) By performing a

time averaging,

**show**that the average power per unit solid angle is: dP e°co's 4 ...### What people are saying - Write a review

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Multipoles Electrostatics of Macroscopic Media | 98 |

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 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