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Page 340
... wave number kD 2 wp KD = 2 ( u2 ) that appreciable departures of the frequency from ∞ , occur . ( 10.106 ) For wave numbers k < kp , the phase and group velocities of the longitudinal plasma oscillations are : ωρ k 3 ( u2 ) Ug Vp ...
... wave number kD 2 wp KD = 2 ( u2 ) that appreciable departures of the frequency from ∞ , occur . ( 10.106 ) For wave numbers k < kp , the phase and group velocities of the longitudinal plasma oscillations are : ωρ k 3 ( u2 ) Ug Vp ...
Page 566
... wave ( kd = = ) and full - wave ( kd = 2 ′′ ) center - fed antennas with two - term multipole expansions ( dashed curves ) . For the half - wave pattern , the dipole approximation ( dotted curve ) is also shown . The agreement between ...
... wave ( kd = = ) and full - wave ( kd = 2 ′′ ) center - fed antennas with two - term multipole expansions ( dashed curves ) . For the half - wave pattern , the dipole approximation ( dotted curve ) is also shown . The agreement between ...
Page 640
... wave solutions , 203 , 212 in wave guide , 244 Uncertainty principle , 209 , 215 use of , to obtain quantum - mechanical modifications , 440 , 442 , 453 , 455 , 511 , 527 , 532 ... Wave packets , spreading in time , 215 Waves , 640 Index.
... wave solutions , 203 , 212 in wave guide , 244 Uncertainty principle , 209 , 215 use of , to obtain quantum - mechanical modifications , 440 , 442 , 453 , 455 , 511 , 527 , 532 ... Wave packets , spreading in time , 215 Waves , 640 Index.
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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 coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ 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