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Page 288
... screen to those of the complementary screen . We first discuss the principle in the scalar Kirchhoff approxi- mation . The diffracting screen is assumed to lie in some surface S which divides space into regions I and II in the sense of ...
... screen to those of the complementary screen . We first discuss the principle in the scalar Kirchhoff approxi- mation . The diffracting screen is assumed to lie in some surface S which divides space into regions I and II in the sense of ...
Page 289
... screen and its comple- ment . We start by considering certain fields E。, B , incident on the screen with metallic surface S ( see Fig . 9.7 ) in otherwise empty space . The presence of the screen gives rise to transmitted and reflected ...
... screen and its comple- ment . We start by considering certain fields E。, B , incident on the screen with metallic surface S ( see Fig . 9.7 ) in otherwise empty space . The presence of the screen gives rise to transmitted and reflected ...
Page 290
... screen . If we substitute for K from ( 9.84 ) , we can write the magnetic induction in region II as B1 ( x ) = 20 x S n × B¿ ( x ' ) G ( x , x ' ) da ( 9.87 ) So This result is identical with ( 9.82 ) except that ( 1 ) the roles of E ...
... screen . If we substitute for K from ( 9.84 ) , we can write the magnetic induction in region II as B1 ( x ) = 20 x S n × B¿ ( x ' ) G ( x , x ' ) da ( 9.87 ) So This result is identical with ( 9.82 ) except that ( 1 ) the roles of E ...
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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