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 19
The righthand side of (1.16) vanishes because dB/dt is finite at the surface and
the area of the loop is zero as the length of the short sides goes to zero. The right
hand side of (1.15) does not vanish, however, if there is an idealized surface ...
The righthand side of (1.16) vanishes because dB/dt is finite at the surface and
the area of the loop is zero as the length of the short sides goes to zero. The right
hand side of (1.15) does not vanish, however, if there is an idealized surface ...
Page 21
The discontinuity formulas (1.19) and (1.20) for E and H are modified, however.
This comes about because the time derivative terms on the righthand sides of (
1.15) and (1.16) no longer vanish. The sweeping of the interface past the
stationary ...
The discontinuity formulas (1.19) and (1.20) for E and H are modified, however.
This comes about because the time derivative terms on the righthand sides of (
1.15) and (1.16) no longer vanish. The sweeping of the interface past the
stationary ...
Page 429
The fields and hence i//(x) will satisfy a radiation condition, With this condition on i
^ at S2 it is easily seen that the contribution from S2 in (9.123) vanishes at least
as the inverse of the radius of the hemisphere or sphere as the radius goes to ...
The fields and hence i//(x) will satisfy a radiation condition, With this condition on i
^ at S2 it is easily seen that the contribution from S2 in (9.123) vanishes at least
as the inverse of the radius of the hemisphere or sphere as the radius goes to ...
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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