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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 = - ( + 1 ) a3Eo ( 4.62 ) ...
... 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 = - ( + 1 ) a3Eo ( 4.62 ) ...
Page 116
... applied field plus that of a dipole at the origin oriented oppositely to the applied field and with dipole moment : 1 p = a3Eo 2 € + 1 . ( 4.66 ) 4.6 Molecular Polarizability and Electric Susceptibility In this section and the next we ...
... applied field plus that of a dipole at the origin oriented oppositely to the applied field and with dipole moment : 1 p = a3Eo 2 € + 1 . ( 4.66 ) 4.6 Molecular Polarizability and Electric Susceptibility In this section and the next we ...
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 ...
Contents
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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