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 50
(c) The electric field at the surface of a conductor is normal to the surface and has
a magnitude 4iro, where <r is the charge density per unit area on the surface. 1.2
The Dirac delta function in three dimensions can be taken as the improper ...
(c) The electric field at the surface of a conductor is normal to the surface and has
a magnitude 4iro, where <r is the charge density per unit area on the surface. 1.2
The Dirac delta function in three dimensions can be taken as the improper ...
Page 169
current corresponds to charges in motion and is described by a current density J,
measured in units of positive charge crossing unit area per unit time, the direction
of motion of the charges denning the direction of J. In electrostatic units, current ...
current corresponds to charges in motion and is described by a current density J,
measured in units of positive charge crossing unit area per unit time, the direction
of motion of the charges denning the direction of J. In electrostatic units, current ...
Page 235
where e is some convenient unit of charge, for example, that of a proton, we can
write (6.101) as (Q')«3 = (a,)a0 + er,,28ap The macroscopic quadrupole density (
6.90) thus becomes Q^ = G* + 1 / Z ern28aP5(x x„)\ Vmolcculei) / where QofJ is ...
where e is some convenient unit of charge, for example, that of a proton, we can
write (6.101) as (Q')«3 = (a,)a0 + er,,28ap The macroscopic quadrupole density (
6.90) thus becomes Q^ = G* + 1 / Z ern28aP5(x x„)\ Vmolcculei) / where QofJ is ...
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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