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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. , Bo 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. , Bo 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 ) = 2 ▽ x So n x B , ( x ' ) G ( x , x ' ) da ( 9.87 ) So This result is identical with ( 9.82 ) except that ( 1 ) the roles of ...
... screen . If we substitute for K from ( 9.84 ) , we can write the magnetic induction in region II as B1 ( x ) = 2 ▽ x So n x B , ( x ' ) G ( x , x ' ) da ( 9.87 ) So This result is identical with ( 9.82 ) except that ( 1 ) the roles of ...
Contents
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ