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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 / ( 1-0 ) 4πnoе2 m ( 7.91 ) ( 7.92 ) k = is called the plasma frequency . Since the wave number can be written as no / c ...
... plasma is governed by equation ( 7.76 ) of Section 7.7 , with plasma ( 7.90 ) inserted for σ : * where k2 * ~ 2 / ( 1-0 ) 4πnoе2 m ( 7.91 ) ( 7.92 ) k = is called the plasma frequency . Since the wave number can be written as no / c ...
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 ...
Page 450
... plasma is divided into two regions . For dimensions large 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 ...
... plasma is divided into two regions . For dimensions large 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 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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