Classical ElectrodynamicsProblems after each chapter |
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Page 91
... integral equations . The general theory of dual integral equations is complicated and not highly developed . But the charged disc problem and variations of it have received considerable attention over the years . H. Weber ( 1873 ) first ...
... integral equations . The general theory of dual integral equations is complicated and not highly developed . But the charged disc problem and variations of it have received considerable attention over the years . H. Weber ( 1873 ) first ...
Page 284
... integral of the first three terms in ( 9.72 ) , involving the product ( GE ) , vanishes identically . To do this we make use of the following easily proved identities connecting surface integrals over a closed surface S to volume integrals ...
... integral of the first three terms in ( 9.72 ) , involving the product ( GE ) , vanishes identically . To do this we make use of the following easily proved identities connecting surface integrals over a closed surface S to volume integrals ...
Page 301
... integral will be large and the integral from the illuminated region will go to zero . As the scattering angle departs from the forward direction the shadow integral will vanish rapidly , both the exponential and the vector factor in the ...
... integral will be large and the integral from the illuminated region will go to zero . As the scattering angle departs from the forward direction the shadow integral will vanish rapidly , both the exponential and the vector factor in the ...
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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