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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 291
... incident fields with the roles of E and B interchanged . The statement of Babinet's principle is therefore as follows : a dif- fracting system consists of a source producing fields E , Bo incident on a thin , plane , perfectly ...
... incident fields with the roles of E and B interchanged . The statement of Babinet's principle is therefore as follows : a dif- fracting system consists of a source producing fields E , Bo incident on a thin , plane , perfectly ...
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 ...
Contents
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ