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 78
charge density become singular as p— *0. For 0 = 2ir (the edge of a thin sheet)
the singularity is as p1'2. This is still integrable so that the charge within a finite
distance from the edge is finite, but it implies that field strengths become very
large ...
charge density become singular as p— *0. For 0 = 2ir (the edge of a thin sheet)
the singularity is as p1'2. This is still integrable so that the charge within a finite
distance from the edge is finite, but it implies that field strengths become very
large ...
Page 109
The radial factor is R(p) = CJm(kp)+DNm(kp) (3.106) If the potential is finite at p =
0, D = 0. The requirement that the potential vanish at p=a means that k can take
on only those special values: km„ = ^, n=l,2,3,... (3.107) where x„„ are the roots of
...
The radial factor is R(p) = CJm(kp)+DNm(kp) (3.106) If the potential is finite at p =
0, D = 0. The requirement that the potential vanish at p=a means that k can take
on only those special values: km„ = ^, n=l,2,3,... (3.107) where x„„ are the roots of
...
Page 333
(a) For fields produced a finite time in the past (and so localized to a finite region
of space) show that, provided the magnetic field is eliminated in favor of the
vector potential A, the angular momentum can be written in the form The first term
is ...
(a) For fields produced a finite time in the past (and so localized to a finite region
of space) show that, provided the magnetic field is eliminated in favor of the
vector potential A, the angular momentum can be written in the form The first term
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