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Page 227
... plasma is governed by equation ( 7.76 ) of Section 7.7 , with plasma ( 7.90 ) inserted for σ : * where k2 - @ 2 ω , 2 m ( 7.91 ) ( 7.92 ) is called the plasma frequency . Since the wave number can be written as no / c , where n is the ...
... plasma is governed by equation ( 7.76 ) of Section 7.7 , with plasma ( 7.90 ) inserted for σ : * where k2 - @ 2 ω , 2 m ( 7.91 ) ( 7.92 ) is called the plasma frequency . Since the wave number can be written as no / c , where n is the ...
Page 329
... plasma with a sharp boundary . Detailed analysis * confirms this qualitative conclusion and sets limits on the quantities involved . It is important to have as little axial field outside the plasma as possible and to keep the plasma ...
... plasma with a sharp boundary . Detailed analysis * confirms this qualitative conclusion and sets limits on the quantities involved . It is important to have as little axial field outside the plasma as possible and to keep the plasma ...
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... plasma is divided into two regions . For dimensions large 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 ...
... plasma is divided into two regions . For dimensions large 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 ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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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