Classical ElectrodynamicsProblems after each chapter |
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Page 232
... incident power ; ( b ) for i greater than the critical angle for total internal reflection , sketch the ratio of transmitted power to incident power as a function of d measured in units of wavelength in the gap . 7.4 A plane polarized ...
... incident power ; ( b ) for i greater than the critical angle for total internal reflection , sketch the ratio of transmitted power to incident power as a function of d measured in units of wavelength in the gap . 7.4 A plane polarized ...
Page 307
... incident on a circular opening of radius a in an otherwise perfectly con- ducting flat screen . The incident wave vector makes an angle « with the normal to the screen . The polarization vector is perpendicular to the plane of incidence ...
... incident on a circular opening of radius a in an otherwise perfectly con- ducting flat screen . The incident wave vector makes an angle « with the normal to the screen . The polarization vector is perpendicular to the plane of incidence ...
Page 429
... incident particle without causing significant deflections , whereas the massive nuclei absorb very little energy but because of their greater charge cause scattering of the incident particle . Thus loss of energy by the incident ...
... incident particle without causing significant deflections , whereas the massive nuclei absorb very little energy but because of their greater charge cause scattering of the incident particle . Thus loss of energy by the incident ...
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Common terms and phrases
4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ