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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 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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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