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... wave is an invariant quantity . Actually , the phase of any plane wave is invariant under a Lorentz transformation , the reason being that the phase can be associated with mere counting which is independent of coordinate frame ...
... wave is an invariant quantity . Actually , the phase of any plane wave is invariant under a Lorentz transformation , the reason being that the phase can be associated with mere counting which is independent of coordinate frame ...
Page
... wave ( kd = π ) 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 = π ) 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 ...
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... 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 |
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