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Page 296
... approximation is dP ( ka ) 2 Pi COS α 4πT cos x + cos 0 ) 22J1 ( ka§ ) ( 9.112 ) kağ dQ where P is given by ( 9.104 ) . i 2 cos α If we compare the vector Kirchhoff result ( 9.103 ) with ( 9.112 ) , we see similarities and differences ...
... approximation is dP ( ka ) 2 Pi COS α 4πT cos x + cos 0 ) 22J1 ( ka§ ) ( 9.112 ) kağ dQ where P is given by ( 9.104 ) . i 2 cos α 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 = # 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 = # 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 ...
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... approximation . Show that the differential cross section for emission of photons per unit solid angle per unit energy interval is 2 R2 = R d20 d ( hw ) dQ 60 he c2 he 2 - hw [ 1 + 2 ( cos 0 ) — P ( cos 0 ) ] 14 284 where 0 is measured ...
... approximation . Show that the differential cross section for emission of photons per unit solid angle per unit energy interval is 2 R2 = R d20 d ( hw ) dQ 60 he c2 he 2 - hw [ 1 + 2 ( cos 0 ) — P ( cos 0 ) ] 14 284 where 0 is measured ...
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Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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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