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Page 227
... plasma is governed by equation ( 7.76 ) of Section 7.7 , with plasma ( 7.90 ) inserted for σ : * k2 མྨཱ ' ( – ' ' ) O ( 7.91 ) where 4πnoе2 = m ( 7.92 ) 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 : * k2 མྨཱ ' ( – ' ' ) O ( 7.91 ) where 4πnoе2 = m ( 7.92 ) is called the plasma frequency . Since the wave number can be written as no / c ...
Page 322
... plasma the pressure p is much too small to resist the magnetic pressure outside . Consequently the radius of the cylinder of plasma is forced inwards ; the plasma column is pinched . This has the desirable consequence that the plasma is ...
... plasma the pressure p is much too small to resist the magnetic pressure outside . Consequently the radius of the cylinder of plasma is forced inwards ; the plasma column is pinched . This has the desirable consequence that the plasma is ...
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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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ