Classical electrodynamicsThis edition refines and improves the first edition. It treats the present experimental limits on the mass of photon and the status of linear superposition, and introduces many other innovations. 
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Page 274
If Ei and E2 have the same phase, (7.19) represents a linearly polarized wave,
with its polarization vector making an angle 6 = tan"1 (E2/Ei) with €i and a
magnitude E = VEi2+E22, as shown in Fig. 7.2. If E] and E2 have different phases
, the ...
If Ei and E2 have the same phase, (7.19) represents a linearly polarized wave,
with its polarization vector making an angle 6 = tan"1 (E2/Ei) with €i and a
magnitude E = VEi2+E22, as shown in Fig. 7.2. If E] and E2 have different phases
, the ...
Page 276
7.4 Electric field and magnetic induction for an elliptically polarized wave.
equivalents. Their measurement determines completely the state of polarization
of the wave. The Stokes parameters can be motivated by observing that for a
wave ...
7.4 Electric field and magnetic induction for an elliptically polarized wave.
equivalents. Their measurement determines completely the state of polarization
of the wave. The Stokes parameters can be motivated by observing that for a
wave ...
Page 414
where the subscripts  and 1 indicate polarization parallel to and perpendicular
to the scattering plane, respectively. The polarization 11(8) of the scattered
radiation is defined by da± do\ d£l dCl From (9.85) we find for the (electric dipole)
...
where the subscripts  and 1 indicate polarization parallel to and perpendicular
to the scattering plane, respectively. The polarization 11(8) of the scattered
radiation is defined by da± do\ d£l dCl From (9.85) we find for the (electric dipole)
...
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Contents
Introduction and Survey  1 
Introduction to Electrostatics  27 
BoundaryValue Problems  54 
Copyright  
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4vector amplitude angle angular distribution angular momentum aperture approximation assumed atomic axis behavior Bessel functions boundary conditions bremsstrahlung calculation Chapter charge density charge q charged particle classical coefficients collision components conductor consider coordinates cross section current density cylinder defined dielectric constant differential diffraction dimensions dipole direction discussed effects electric and magnetic electric field electromagnetic fields electrons electrostatic energy loss expansion expression factor finite force frequency given Green function incident integral Lagrangian limit linear Lorentz transformation macroscopic magnetic field magnetic induction magnitude Maxwell equations medium modes molecules multipole multipole expansion multipole moments nonrelativistic normal obtain oscillations parallel parameter photon Phys plane wave plasma point charge polarization problem propagation quantum quantummechanical radius region relativistic resonant rest frame result scalar scalar potential scattering shown in Fig solution spectrum sphere spherical surface tensor theorem transverse unit vanishes vector potential velocity wave guide wave number wavelength written zero