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 447
9.13 Scattering in the ShortWavelength Limit Scattering in the longwavelength
limit has been discussed in Sections 9.6 and 9.7. The opposite limit, similar to the
Kirchhoff domain of diffraction, is a scattering by obstacles large compared to a ...
9.13 Scattering in the ShortWavelength Limit Scattering in the longwavelength
limit has been discussed in Sections 9.6 and 9.7. The opposite limit, similar to the
Kirchhoff domain of diffraction, is a scattering by obstacles large compared to a ...
Page 774
We specialize now to the longwavelength limit (kaŤ 1) for a perfectly conducting
sphere (Z, = 0), and leave examples of slightly more complexity to the problems.
Only the 1= 1 terms in (16.147) are important. From (16.153) we find ...
We specialize now to the longwavelength limit (kaŤ 1) for a perfectly conducting
sphere (Z, = 0), and leave examples of slightly more complexity to the problems.
Only the 1= 1 terms in (16.147) are important. From (16.153) we find ...
Page 778
Tabulate the wavelength (defined in terms of the real part of the frequency) in
units of the radius a and the decay time (defined as the time taken for the energy
to fall to e~' of its initial value) in units of the transit time (ale) for each of the
modes.
Tabulate the wavelength (defined in terms of the real part of the frequency) in
units of the radius a and the decay time (defined as the time taken for the energy
to fall to e~' of its initial value) in units of the transit time (ale) for each of the
modes.
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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