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Page 479
... ΦΩ 0 ΦΩ ( 14.58 ) defines a quantity dl ( w ) / d§ which is the energy radiated per unit solid angle per unit frequency interval : dl ( w ) ΦΩ = | A ( @ ) 2 + | A ( w ) | 2 ( 14.59 ) If A ( t ) is real , from ( 14.55 ) it is evident ...
... ΦΩ 0 ΦΩ ( 14.58 ) defines a quantity dl ( w ) / d§ which is the energy radiated per unit solid angle per unit frequency interval : dl ( w ) ΦΩ = | A ( @ ) 2 + | A ( w ) | 2 ( 14.59 ) If A ( t ) is real , from ( 14.55 ) it is evident ...
Page 485
... ΦΩ 10 = 0 ~ 3 e2 γι 2п с · 22 ω 2w / wc We ( 14.88 ) These limiting forms show that the spectrum at 00 increases ... ΦΩ ΦΩ 10 = 0 ( 14.90 ) Thus the critical angle , defined by the 1 / [ Sect . 14.6 ] 485 Radiation by Moving Charges.
... ΦΩ 10 = 0 ~ 3 e2 γι 2п с · 22 ω 2w / wc We ( 14.88 ) These limiting forms show that the spectrum at 00 increases ... ΦΩ ΦΩ 10 = 0 ( 14.90 ) Thus the critical angle , defined by the 1 / [ Sect . 14.6 ] 485 Radiation by Moving Charges.
Page 501
... ΦΩ есва sin20 cos2 ( wt ' ) 4a2 ( 1 + cos 0 sin wot ́ ) 5 ( b ) By performing a time averaging , show that the average power per unit solid angle is : dP ΦΩ 32πα | ( 1 e2cB4 4 + B2 cos2 0 B2 cos2 0 ) sin2 0 - ( c ) Make rough sketches ...
... ΦΩ есва sin20 cos2 ( wt ' ) 4a2 ( 1 + cos 0 sin wot ́ ) 5 ( b ) By performing a time averaging , show that the average power per unit solid angle is : dP ΦΩ 32πα | ( 1 e2cB4 4 + B2 cos2 0 B2 cos2 0 ) sin2 0 - ( c ) Make rough sketches ...
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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