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 319
behavior of n(w) and the location of its poles and branch cuts needs to be
considered for an accurate description of the amplitude. In general the amplitude
remains very small, however. Only when the elapsed time reaches f1 = k'(0)x ...
behavior of n(w) and the location of its poles and branch cuts needs to be
considered for an accurate description of the amplitude. In general the amplitude
remains very small, however. Only when the elapsed time reaches f1 = k'(0)x ...
Page 320
First Precursor A more accurate expression than (7.139) for the amplitude at early
times can be obtained following Sommerfeld. We have seen that the amplitude at
times soon after t = to is determined by the behavior of the integrand in (7.124) ...
First Precursor A more accurate expression than (7.139) for the amplitude at early
times can be obtained following Sommerfeld. We have seen that the amplitude at
times soon after t = to is determined by the behavior of the integrand in (7.124) ...
Page 324
The amplitude will then be given accurately by an integration only over the
contours wrapped around the singularities of A(&>). For example, we consider an
incident wave of the form u,(0, t) = 0(t)e"" sin (0 vt) (7.149) where 0(t) is the step ...
The amplitude will then be given accurately by an integration only over the
contours wrapped around the singularities of A(&>). For example, we consider an
incident wave of the form u,(0, t) = 0(t)e"" sin (0 vt) (7.149) where 0(t) is the step ...
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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