Classical ElectrodynamicsProblems after each chapter |
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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 ) a2E Eo ( 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 ) a2E Eo ( 4.62 ) ...
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 ...
Page 310
John David Jackson. balance between the applied force and the frictional drag . When the frequency of the applied fields is comparable to v , the electrons have time to accelerate and decelerate between collisions . Then inertial effects ...
John David Jackson. balance between the applied force and the frictional drag . When the frequency of the applied fields is comparable to v , the electrons have time to accelerate and decelerate between collisions . Then inertial effects ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ