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Page 280
... Kirchhoff ( 1882 ) , based on the ideas of superposition of elemental wavelets due to Huygens . In this section we will discuss Kirchhoff's method and point out some of its deficiencies , and in the next section derive vector theorems ...
... Kirchhoff ( 1882 ) , based on the ideas of superposition of elemental wavelets due to Huygens . In this section we will discuss Kirchhoff's method and point out some of its deficiencies , and in the next section derive vector theorems ...
Page 283
... Kirchhoff approximation works best in the short - wavelength limit in which the diffracting openings have dimensions ... Kirchhoff integral ( 9.65 ) . 9.6 Vector Equivalents of Kirchhoff Integral To obtain vector equivalents to the ...
... Kirchhoff approximation works best in the short - wavelength limit in which the diffracting openings have dimensions ... Kirchhoff integral ( 9.65 ) . 9.6 Vector Equivalents of Kirchhoff Integral To obtain vector equivalents to the ...
Page 307
... Kirchhoff relation ( 9.82 ) , assuming that the tangential electric field in the opening is the incident unperturbed field . ( b ) Calculate the corresponding result of the scalar Kirchhoff approxi- mation . = ( c ) For b = a , B = 45 ...
... Kirchhoff relation ( 9.82 ) , assuming that the tangential electric field in the opening is the incident unperturbed field . ( b ) Calculate the corresponding result of the scalar Kirchhoff approxi- mation . = ( c ) For b = a , B = 45 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ