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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Results 13 of 67
Page 647
Fig. 13.9 Atomic scattering, including effects of electronic screening at small
angles and finite nuclear size at large angles. (13.96) over all solid angle: f da .
This yields «"*2„(^)T_£fyF (13.103, (2zZe2\2 1 2/2zZe2V (13.104) where the final
form ...
Fig. 13.9 Atomic scattering, including effects of electronic screening at small
angles and finite nuclear size at large angles. (13.96) over all solid angle: f da .
This yields «"*2„(^)T_£fyF (13.103, (2zZe2\2 1 2/2zZe2V (13.104) where the final
form ...
Page 648
The complete distribution in angle can be approximated by considering the two
regions separately. The intermediate region of socalled plural scattering must
allow a smooth transition from small to large angles. The important quantity in the
...
The complete distribution in angle can be approximated by considering the two
regions separately. The intermediate region of socalled plural scattering must
allow a smooth transition from small to large angles. The important quantity in the
...
Page 676
We note that the lowfrequency components are emitted at much wider angles
than the average, (02}"2~y_1. In the highfrequency limit (to>o)c), £(0) is large
compared to unity. Then the intensity falls off in angle approximately as d2I d2I da
) dil ...
We note that the lowfrequency components are emitted at much wider angles
than the average, (02}"2~y_1. In the highfrequency limit (to>o)c), £(0) is large
compared to unity. Then the intensity falls off in angle approximately as d2I d2I da
) dil ...
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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