Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 15
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 ...
... 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 ...
Page 290
... screen . If we substitute for K from ( 9.84 ) , we can write the magnetic induction in region II as B , ( x ) = 2V x S nx B , ( x ' ) G ( x , x ' ) da ( 9.87 ) Sa 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 B , ( x ) = 2V x S nx B , ( x ' ) G ( x , x ' ) da ( 9.87 ) Sa This result is identical with ( 9.82 ) except that ( 1 ) the roles of E ...
Other editions - View all
Common terms and phrases
4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ