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 269
Then comes a simplified discussion of propagation in the ionosphere, and of
waves in a conducting or dissipative medium. The ideas of phase and group
velocities and the spreading of a pulse or wave packet as it propagates in a
dispersive ...
Then comes a simplified discussion of propagation in the ionosphere, and of
waves in a conducting or dissipative medium. The ideas of phase and group
velocities and the spreading of a pulse or wave packet as it propagates in a
dispersive ...
Page 270
infinite medium are: VE = 0 VxE+^ = 0 c dt VB = 0 VxB^ = 0 C dt (7.1) where
the medium is characterized by the parameters jx, e, assumed for the moment to
be independent of frequency. By combining the two curl equations and making
use ...
infinite medium are: VE = 0 VxE+^ = 0 c dt VB = 0 VxB^ = 0 C dt (7.1) where
the medium is characterized by the parameters jx, e, assumed for the moment to
be independent of frequency. By combining the two curl equations and making
use ...
Page 685
It was shown in Section 13.5, however, that a particle moving at constant velocity
can radiate if it is in a material medium and is moving with a speed greater than
the phase velocity of light in that medium. This radiation, with its characteristic ...
It was shown in Section 13.5, however, that a particle moving at constant velocity
can radiate if it is in a material medium and is moving with a speed greater than
the phase velocity of light in that medium. This radiation, with its characteristic ...
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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