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Page 38
... inversion is a . The inversion of the surface S is the surface S ' , and vice versa . not . The only exception occurs when Ø vanishes on some surface . Then ' also vanishes on the inverted surface . One might think that , since P is ...
... inversion is a . The inversion of the surface S is the surface S ' , and vice versa . not . The only exception occurs when Ø vanishes on some surface . Then ' also vanishes on the inverted surface . One might think that , since P is ...
Page 39
... inversion and associated parameters we can obtain the potential due to a point charge q a distance d away from an infinite , grounded , conducting plane . Evidently , if the center of inversion O is chosen to lie on the surface of the ...
... inversion and associated parameters we can obtain the potential due to a point charge q a distance d away from an infinite , grounded , conducting plane . Evidently , if the center of inversion O is chosen to lie on the surface of the ...
Page 53
... inversion radius . ( c ) What is the physical situation described by the inverted solution if the center of inversion lies inside the conducting sphere ? 2.10 Knowing that the capacitance of a thin , flat , circular , conducting disc of ...
... inversion radius . ( c ) What is the physical situation described by the inverted solution if the center of inversion lies inside the conducting sphere ? 2.10 Knowing that the capacitance of a thin , flat , circular , conducting disc of ...
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