Classical Electrodynamics |
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Page 115
... applied field with magnitude 3 Ein = Eo < Eo € + 2 ( 4.61 ) Outside the sphere the potential is equivalent to the applied field E。 plus the field of an electric dipole at the origin with dipole moment : P = a3Eo ( 4.62 ) oriented in ...
... applied field with magnitude 3 Ein = Eo < Eo € + 2 ( 4.61 ) Outside the sphere the potential is equivalent to the applied field E。 plus the field of an electric dipole at the origin with dipole moment : P = a3Eo ( 4.62 ) oriented in ...
Page 116
... applied field plus that of a dipole at the origin oriented oppositely to the applied field and with dipole moment : € - P = 2 € + 1 . a3E 。 Eo ( 4.66 ) 4.6 Molecular Polarizability and Electric Susceptibility In this section and the ...
... applied field plus that of a dipole at the origin oriented oppositely to the applied field and with dipole moment : € - P = 2 € + 1 . a3E 。 Eo ( 4.66 ) 4.6 Molecular Polarizability and Electric Susceptibility In this section and the ...
Page 309
... applied to the solid conductor , but mass motion does not in general occur . The effects of the applied fields on the atoms themselves are taken up as stresses in the lattice structure . For a fluid , on the other hand , the fields act ...
... applied to the solid conductor , but mass motion does not in general occur . The effects of the applied fields on the atoms themselves are taken up as stresses in the lattice structure . For a fluid , on the other hand , the fields act ...
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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