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Page 82
... radius b . Poisson integral ( 2.25 ) . The equivalence of this solution to the Green's function expansion solution ... radius b with a concentric ring of charge of radius a and total charge Q. The ring of charge is located in the x - y ...
... radius b . Poisson integral ( 2.25 ) . The equivalence of this solution to the Green's function expansion solution ... radius b with a concentric ring of charge of radius a and total charge Q. The ring of charge is located in the x - y ...
Page 166
... radius a has a hole of radius b bored parallel to , and centered a distance d from , the cylinder axis ( d + b < Ia ) . The current density is uniform throughout the remaining metal of the cylinder and is parallel to the axis . Use ...
... radius a has a hole of radius b bored parallel to , and centered a distance d from , the cylinder axis ( d + b < Ia ) . The current density is uniform throughout the remaining metal of the cylinder and is parallel to the axis . Use ...
Page 576
... radius a in a conducting medium can serve as an electromagnetic resonant cavity . ( a ) Assuming infinite conductivity , determine the transcendental equations for the characteristic frequencies win of the cavity for TE and TM modes ...
... radius a in a conducting medium can serve as an electromagnetic resonant cavity . ( a ) Assuming infinite conductivity , determine the transcendental equations for the characteristic frequencies win of the cavity for TE and TM modes ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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 coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ 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