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 25
For macroscopic situations where 10"7cm is a negligible distance, we can
idealize the charge density and electric field behavior as p(x) = a8(x) and EK(x) =
4vad(x), corresponding to a truly surface density and a stepfunction jump of the
field.
For macroscopic situations where 10"7cm is a negligible distance, we can
idealize the charge density and electric field behavior as p(x) = a8(x) and EK(x) =
4vad(x), corresponding to a truly surface density and a stepfunction jump of the
field.
Page 144
In the Introduction we indicated the need for averaging over macroscopically
small, but microscopically large, regions in order to obtain the Maxwell equations
appropriate for macroscopic phenomena. This is done in a careful fashion in ...
In the Introduction we indicated the need for averaging over macroscopically
small, but microscopically large, regions in order to obtain the Maxwell equations
appropriate for macroscopic phenomena. This is done in a careful fashion in ...
Page 232
The detailed extent of the molecular charge distribution is important at the
microscopic level, of course, but is replaced in its effect by a sum of multipoles for
macroscopic phenomena. The total microscopic charge density (6.79) consists of
the ...
The detailed extent of the molecular charge distribution is important at the
microscopic level, of course, but is replaced in its effect by a sum of multipoles for
macroscopic phenomena. The total microscopic charge density (6.79) consists of
the ...
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Contents
Introduction and Survey  1 
Introduction to Electrostatics  27 
BoundaryValue Problems  54 
Copyright  
18 other sections not shown
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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