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Page 248
... gives the time - averaged flux of energy . For the two types of field we find , using ( 8.24 ) : S = wk [ [ [ G / 01x2 + 1 i i 2 γι k 0 • ] ( 8.48 ) [ H [ SION - 122 + VIN ] k 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 ) : S = wk [ [ [ G / 01x2 + 1 i i 2 γι k 0 • ] ( 8.48 ) [ H [ SION - 122 + VIN ] k 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 366
... gives the anomalous Zeeman effect correctly , but has a spin - orbit interaction which is twice too large . The error in ( 11.45 ) can be traced to the incorrectness of ( 11.40 ) as an equation of motion for the electron spin . The left ...
... gives the anomalous Zeeman effect correctly , but has a spin - orbit interaction which is twice too large . The error in ( 11.45 ) can be traced to the incorrectness of ( 11.40 ) as an equation of motion for the electron spin . The left ...
Contents
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ