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 32
1.4 Differential Form of Gauss's Law Gauss's law can be thought of as being an
integral formulation of the law of electrostatics. We can obtain a differential form (
i.e., a differential equation) by using the divergence theorem. The divergence ...
1.4 Differential Form of Gauss's Law Gauss's law can be thought of as being an
integral formulation of the law of electrostatics. We can obtain a differential form (
i.e., a differential equation) by using the divergence theorem. The divergence ...
Page 87
We write down the differential equation for Pi(x), multiply by P(x), and then
integrate over the interval: Jl, Pr(x)(^[(1~x2)^]+ia+1)p,(x)} dx=0 (317) Integrating
the first term by parts, we obtain I', [(x2D^!^:+'(i+l)Pr(x)Pl(x)]dx = 0 (3.18) If we
now write ...
We write down the differential equation for Pi(x), multiply by P(x), and then
integrate over the interval: Jl, Pr(x)(^[(1~x2)^]+ia+1)p,(x)} dx=0 (317) Integrating
the first term by parts, we obtain I', [(x2D^!^:+'(i+l)Pr(x)Pl(x)]dx = 0 (3.18) If we
now write ...
Page 413
With (9.80) and (9.79), the differential cross section can be written da k4 ^ (n, e;
no, «o)=g2 «* • p+(nxe*) • m (9.82) The dependence of the cross section on n„
and Co is implicitly contained in the dipole moments p and m. The variation of ...
With (9.80) and (9.79), the differential cross section can be written da k4 ^ (n, e;
no, «o)=g2 «* • p+(nxe*) • m (9.82) The dependence of the cross section on n„
and Co is implicitly contained in the dipole moments p and m. The variation of ...
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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