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 698
operation, show that the power spectrum, averaged over one cycle of operation,
is where x = 2Wio,.„ (b) Determine Umiting forms for the spectrum when x« 1 and
x»l. (c) By finding tables of the integral (it is an incomplete gamma function) or by
...
operation, show that the power spectrum, averaged over one cycle of operation,
is where x = 2Wio,.„ (b) Determine Umiting forms for the spectrum when x« 1 and
x»l. (c) By finding tables of the integral (it is an incomplete gamma function) or by
...
Page 725
Of course, as has already been observed in Section 15.2(d), such soft photons
transform into energetic photons in the laboratory. But the spectrum of virtual
quanta contains frequencies up to a)'—yMc2/h. For such frequencies the
scattering of ...
Of course, as has already been observed in Section 15.2(d), such soft photons
transform into energetic photons in the laboratory. But the spectrum of virtual
quanta contains frequencies up to a)'—yMc2/h. For such frequencies the
scattering of ...
Page 729
Then the spectrum is a typical bremsstrahlung spectrum. But for w = w0 the
intensity is very large (infinite in our approximation). The behavior of the photon
spectrum is shown in Fig. 15.11. The singularity at w = w0 may seem alarming,
but it is ...
Then the spectrum is a typical bremsstrahlung spectrum. But for w = w0 the
intensity is very large (infinite in our approximation). The behavior of the photon
spectrum is shown in Fig. 15.11. The singularity at w = w0 may seem alarming,
but it is ...
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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