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 370
(a) Orthonormal Modes To facilitate the handling of the expansion of fields in the
normal modes, it is useful to standardize the notation for the fields of a given
mode, treating TE and TM modes on an equal footing and introducing a
convenient ...
(a) Orthonormal Modes To facilitate the handling of the expansion of fields in the
normal modes, it is useful to standardize the notation for the fields of a given
mode, treating TE and TM modes on an equal footing and introducing a
convenient ...
Page 439
9.12 A diffraction screen S„ and its complementary diffraction screen Sk. If there
are sources inside S (in region I) which give rise to a field ^i(x), then in the
absence of either screen the field i/»(x) in region II is given by the Kirchhoff
integral ...
9.12 A diffraction screen S„ and its complementary diffraction screen Sk. If there
are sources inside S (in region I) which give rise to a field ^i(x), then in the
absence of either screen the field i/»(x) in region II is given by the Kirchhoff
integral ...
Page 496
Detailed calculations show that the damping can be expressed in terms of an
imaginary part of the frequency given by provided k«kD. To obtain (10.93) a
Maxwellian distribution of velocities was assumed. For kskD the damping
constant is ...
Detailed calculations show that the damping can be expressed in terms of an
imaginary part of the frequency given by provided k«kD. To obtain (10.93) a
Maxwellian distribution of velocities was assumed. For kskD the damping
constant is ...
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Contents
Introduction and Survey  1 
Introduction to Electrostatics  27 
BoundaryValue Problems  54 
Copyright  
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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