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Page 297
... compared in Fig . 9.11 for the angle of incidence equal to 45 ° and for an aperture one wave- length in diameter ... compared to a wavelength , an entirely different approach is necessary . We will consider a thin , flat , perfectly ...
... compared in Fig . 9.11 for the angle of incidence equal to 45 ° and for an aperture one wave- length in diameter ... compared to a wavelength , an entirely different approach is necessary . We will consider a thin , flat , perfectly ...
Page 432
... compared to the orbital period of motion , it may be expected that the collision will be sudden enough that the electron may be treated as free . If , on the other hand , the collision time ( 11.120 ) is very long compared to the ...
... compared to the orbital period of motion , it may be expected that the collision will be sudden enough that the electron may be treated as free . If , on the other hand , the collision time ( 11.120 ) is very long compared to the ...
Page 450
... compared to the Debye screening distance k1 ( 10.106 ) , the plasma acts as a continuous medium in which the charged particles participate in collective behavior such as plasma oscillations . For dimensions small compared to k1 ...
... compared to the Debye screening distance k1 ( 10.106 ) , the plasma acts as a continuous medium in which the charged particles participate in collective behavior such as plasma oscillations . For dimensions small compared to k1 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle coefficients collisions component conducting conductor consider 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave 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 number wavelength ΦΩ