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Page 210
... wave number . The pulse shown at t = 0 in Fig . 7.5 begins to move as time goes on . The different frequency or wave - number components in it move at different phase velocities . Consequently there is a tendency for the original ...
... wave number . The pulse shown at t = 0 in Fig . 7.5 begins to move as time goes on . The different frequency or wave - number components in it move at different phase velocities . Consequently there is a tendency for the original ...
Page 245
... wave number k is determined for each value of λ : @ 2 k22 2 = με — If we define a cutoff frequency w ( 8.37 ) ( 8.38 ) * @ 2 = = [ c ] Τ με then the wave number can be written : kλ = ― ( 8.39 ) * We note that , for w > w , the wave ...
... wave number k is determined for each value of λ : @ 2 k22 2 = με — If we define a cutoff frequency w ( 8.37 ) ( 8.38 ) * @ 2 = = [ c ] Τ με then the wave number can be written : kλ = ― ( 8.39 ) * We note that , for w > w , the wave ...
Page 340
John David Jackson. closely ww . It is only for wave numbers comparable to the Debye wave number kD ' KD 2 = ωρ 2 ( u ) ( 10.106 ) that appreciable departures of the frequency from @ , occur . For wave numbers k « k » , the phase and ...
John David Jackson. closely ww . It is only for wave numbers comparable to the Debye wave number kD ' KD 2 = ωρ 2 ( u ) ( 10.106 ) that appreciable departures of the frequency from @ , occur . For wave numbers k « k » , the phase and ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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