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Page 251
... frequency dependence . Thus , using ( 8.59 ) with ( 8.62 ) and ( 8.51 ) , plus the frequency dependence of the skin depth ( 7.85 ) , we find 1/2 ( 1 ) Pi = [ + ] 1 C μ σδι 2A 21⁄2 [ & + n ( 2 ) ] ( 8.63 ) * @ 2 where σ is the ...
... frequency dependence . Thus , using ( 8.59 ) with ( 8.62 ) and ( 8.51 ) , plus the frequency dependence of the skin depth ( 7.85 ) , we find 1/2 ( 1 ) Pi = [ + ] 1 C μ σδι 2A 21⁄2 [ & + n ( 2 ) ] ( 8.63 ) * @ 2 where σ is the ...
Page 310
... frequencies well above the collision frequency another thing happens . The electrons and ions are accelerated in opposite directions by electric fields and tend to separate . Strong electrostatic restoring forces are set up by this ...
... frequencies well above the collision frequency another thing happens . The electrons and ions are accelerated in opposite directions by electric fields and tend to separate . Strong electrostatic restoring forces are set up by this ...
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... frequency spectrum thus contains frequencies up to a maximum w , ~ ~ ( At ) -1 . for arbitrary motion it plays the role of a fundamental frequency of motion . Equation ( 14.50 ) shows that a relativistic particle emits a broad spectrum ...
... frequency spectrum thus contains frequencies up to a maximum w , ~ ~ ( At ) -1 . for arbitrary motion it plays the role of a fundamental frequency of motion . Equation ( 14.50 ) shows that a relativistic particle emits a broad spectrum ...
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