Classical Electrodynamics |
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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 vanishes on some surface . Then ' also vanishes on the inverted surface . 0 One might think that , since is ...
... inversion is a . The inversion of the surface S is the surface S ' , and vice versa . not . The only exception occurs when vanishes on some surface . Then ' also vanishes on the inverted surface . 0 One might think that , since 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 ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss factor force equation frame 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 P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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