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Page 248
... gives the time - averaged flux of energy . For the two types of field we find , using ( 8.24 ) : wk S = 8πγ [ [ [ GIVIN2 + 12 DIN • ] i ¥ ▽ t ¥ * k i ¡ 22 ¥ * ▽ t ¥ k ( 8.48 ) where the upper ( lower ) line is for TM ( TE ) modes ...
... gives the time - averaged flux of energy . For the two types of field we find , using ( 8.24 ) : wk S = 8πγ [ [ [ GIVIN2 + 12 DIN • ] i ¥ ▽ t ¥ * k i ¡ 22 ¥ * ▽ t ¥ k ( 8.48 ) where the upper ( lower ) line is for TM ( TE ) modes ...
Page 273
... gives a transverse magnetic induction and the other of which gives a transverse electric field . These physically distinct contributions can be [ Sect . 9.3 ] 273 Simple Radiating Systems and Diffraction Magnetic dipole and quadrupole ...
... gives a transverse magnetic induction and the other of which gives a transverse electric field . These physically distinct contributions can be [ Sect . 9.3 ] 273 Simple Radiating Systems and Diffraction Magnetic dipole and quadrupole ...
Page
... gives an energy transfer large compared to typical atomic excitation energies would we expect it to be correct . This would set quite a different upper limit on the impact parameters . Fortunately the classical result can be applied in ...
... gives an energy transfer large compared to typical atomic excitation energies would we expect it to be correct . This would set quite a different upper limit on the impact parameters . Fortunately the classical result can be applied in ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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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