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Page 296
... approximation is dP ΦΩ d Pi ( ka ) 2 4π COS a cos x + cos 0 2J1 ( kağ ) 2 cos x kağ 2 ( 9.112 ) where P , is given by ( 9.104 ) . If we compare the vector Kirchhoff result ( 9.103 ) with ( 9.112 ) , we see similarities and differences ...
... approximation is dP ΦΩ d Pi ( ka ) 2 4π COS a cos x + cos 0 2J1 ( kağ ) 2 cos x kağ 2 ( 9.112 ) where P , is given by ( 9.104 ) . If we compare the vector Kirchhoff result ( 9.103 ) with ( 9.112 ) , we see similarities and differences ...
Page 297
... approximation in each case . We see that for ka = π there is a considerable disagreement between the two approximations . There is reason to believe that the vector Kirchhoff result is close to the correct one , even though the ...
... approximation in each case . We see that for ka = π there is a considerable disagreement between the two approximations . There is reason to believe that the vector Kirchhoff result is close to the correct one , even though the ...
Page 535
... approximation . Show that the differential cross section for emission of photons per unit solid angle per unit energy interval is d20 R2 ( q2 v2 R d ( hw ) d 60 he c2 he = 2 - hw [ 1 + P2 ( cos 0 ) — P4 ( cos 0 ) ] 14 where is measured ...
... approximation . Show that the differential cross section for emission of photons per unit solid angle per unit energy interval is d20 R2 ( q2 v2 R d ( hw ) d 60 he c2 he = 2 - hw [ 1 + P2 ( cos 0 ) — P4 ( cos 0 ) ] 14 where is measured ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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 coefficients collisions component conducting conductor consider 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave 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 number wavelength ΦΩ