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Page 225
... simple consequence is that the high - frequency inductance of circuit elements is somewhat smaller than the low - frequency inductance because of the expulsion of flux from the interior of the conductors . The problem of reflection and ...
... simple consequence is that the high - frequency inductance of circuit elements is somewhat smaller than the low - frequency inductance because of the expulsion of flux from the interior of the conductors . The problem of reflection and ...
Page 268
... simple radiating systems . A more systematic approach to radiation by localized distributions of charge and current is left to Chapter 16 , where multipole fields are discussed . The second half of the chapter is devoted to the subject ...
... simple radiating systems . A more systematic approach to radiation by localized distributions of charge and current is left to Chapter 16 , where multipole fields are discussed . The second half of the chapter is devoted to the subject ...
Page 277
... simple that integral ( 9.3 ) for the vector potential can be found in relatively simple , closed form . As an example of such a system we consider a thin , linear antenna of length d which is excited across a small gap at its mid- point ...
... simple that integral ( 9.3 ) for the vector potential can be found in relatively simple , closed form . As an example of such a system we consider a thin , linear antenna of length d which is excited across a small gap at its mid- point ...
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