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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 458
... gives a single - scattering distribution for the projected angle : Ps ( 0 ' ) do ' = Nt do ' = Nt do do ' 2 2zZe2 2 do ' pv 0/3 ( 13.113 ) ( 13.114 ) The single - scattering distribution is valid only for angles large compared to ( 2 ) ...
... gives a single - scattering distribution for the projected angle : Ps ( 0 ' ) do ' = Nt do ' = Nt do do ' 2 2zZe2 2 do ' pv 0/3 ( 13.113 ) ( 13.114 ) The single - scattering distribution is valid only for angles large compared to ( 2 ) ...
Page 531
... gives rise to radiation , but with a spectrum of quite different character . The intensity distribution in angle and frequency for a point magnetic moment in motion is given by ( 14.74 ) . The electronic magnetic moment can be treated ...
... gives rise to radiation , but with a spectrum of quite different character . The intensity distribution in angle and frequency for a point magnetic moment in motion is given by ( 14.74 ) . The electronic magnetic moment can be treated ...
Contents
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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