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Page 296
... approximation is dP ( ka ) 2 cos α + cos 0 Pi i ΦΩ COS α 2 ) * 4πT 2 cos a 2J1 ( ka§ ) kağ ( 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 ...
... approximation is dP ( ka ) 2 cos α + cos 0 Pi i ΦΩ COS α 2 ) * 4πT 2 cos a 2J1 ( ka§ ) kağ ( 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 ...
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 ...
... 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 ...
Page 628
... approximation in , 282 scalar Huygens - Kirchhoff theory of , 280 Smythe's vector theorem for , 287 use of Green's theorem in , 281 , 283 vector Kirchhoff approximation , 285 Diffusion of magnetic fields , 313 Diffusion time of magnetic ...
... approximation in , 282 scalar Huygens - Kirchhoff theory of , 280 Smythe's vector theorem for , 287 use of Green's theorem in , 281 , 283 vector Kirchhoff approximation , 285 Diffusion of magnetic fields , 313 Diffusion time of magnetic ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ