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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 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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