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... 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 ...
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... 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 ...
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... compared to the Debye screening distance k ̄1 ( 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 k ̄1 ( 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 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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