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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 ~ 1/2 ( 1-2 ) ( 7.91 ) where @ , 2 = m ( 7.92 ) is called the plasma frequency . Since the wave number can be written as k = nw / c ...
... plasma is governed by equation ( 7.76 ) of Section 7.7 , with plasma ( 7.90 ) inserted for σ : * k2 ~ 1/2 ( 1-2 ) ( 7.91 ) where @ , 2 = m ( 7.92 ) is called the plasma frequency . Since the wave number can be written as k = nw / 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 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ