## Classical electrodynamics |

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Page 233

(c)

coefficient is T = - 2e-2,l<> cos (2//<5) + e-^9 Sketch log T as a function of (</<5),

assuming Re ft = Define "very small thickness." 7.6 Plane waves propagate in a ...

(c)

**Show**that, except for sheets of very small thickness, the transmissioncoefficient is T = - 2e-2,l<> cos (2//<5) + e-^9 Sketch log T as a function of (</<5),

assuming Re ft = Define "very small thickness." 7.6 Plane waves propagate in a ...

Page 501

(a)

e2cp sin2 6 cos2 (eop rfQ " 4«z2 (1 + p cos 6 sin ay')5 where ft = aw0/c. (b) By

performing a time averaging,

dP ...

(a)

**Show**that the instantaneous power radiated per unit solid angle is: dP(t') ^e2cp sin2 6 cos2 (eop rfQ " 4«z2 (1 + p cos 6 sin ay')5 where ft = aw0/c. (b) By

performing a time averaging,

**show**that the average power per unit solid angle is:dP ...

Page 503

(b)

radiated only into multiples of Mo0, but with an intensity A'2 times that for a single

charge. Give a qualitative explanation of these facts. (c) Without detailed ...

(b)

**Show**that, if the charges are uniformly spaced around the circle, energy isradiated only into multiples of Mo0, but with an intensity A'2 times that for a single

charge. Give a qualitative explanation of these facts. (c) Without detailed ...

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### Contents

Introduction to Electrostatics | 1 |

Scalar potential | 7 |

Greens theorem | 14 |

Copyright | |

17 other sections not shown

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### Common terms and phrases

4-vector acceleration angular distribution approximation assumed atomic average axis behavior Bessel functions boundary conditions bremsstrahlung calculate Chapter charge density charge q charged particle classical coefficients collisions component conductor Consequently consider coordinates cross section current density cylinder defined delta function dielectric constant diffraction dimensions dipole direction discussed effects electric field electromagnetic fields electron electrostatic emitted energy loss expansion expression factor force equation frequency given Green's function impact parameter incident particle inside integral Laplace's equation limit linear Lorentz invariant Lorentz transformation macroscopic magnetic field magnetic induction magnitude Maxwell's equations meson molecules momentum multipole multipole expansion nonrelativistic obtain orbit oscillations parallel perpendicular photon plane wave plasma point charge polarization power radiated problem quantum quantum-mechanical radiative radius region relativistic result scalar scattering shown in Fig shows solid angle solution spectrum spherical surface theorem transverse vanishes vector potential wave equation wave number wavelength written zero