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Page 227
... simple result ( 7.93 ) for the index of refraction of a plasma is modified by the presence of an external static magnetic induction . This circumstance arises not only in the laboratory , but also in the ionosphere , where the earth's ...
... simple result ( 7.93 ) for the index of refraction of a plasma is modified by the presence of an external static magnetic induction . This circumstance arises not only in the laboratory , but also in the ionosphere , where the earth's ...
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
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ 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 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ