Classical Electrodynamics |
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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 2 ( -1 ) m ( 7.91 ) ( 7.92 ) is called the plasma frequency . Since the wave number can be written as k = 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 2 ( -1 ) m ( 7.91 ) ( 7.92 ) is called the plasma frequency . Since the wave number can be written as k = no / c , where n is the ...
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 343
... plasma oscillations . It is a happy and not fortuitous happening that plasma oscillations of shorter wavelengths can independently be shown not to exist because of severe damping . REFERENCES AND SUGGESTED READING The subject of ...
... plasma oscillations . It is a happy and not fortuitous happening that plasma oscillations of shorter wavelengths can independently be shown not to exist because of severe damping . REFERENCES AND SUGGESTED READING The subject of ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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