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 139
The first concerns the relationship of the Cartesian multipole moments like (4.8)
to the spherical multipole moments (4.3). The former are (I+l)(l+2)/2 in number
and for I>1 are more numerous than the (21+1) spherical components. There is
no ...
The first concerns the relationship of the Cartesian multipole moments like (4.8)
to the spherical multipole moments (4.3). The former are (I+l)(l+2)/2 in number
and for I>1 are more numerous than the (21+1) spherical components. There is
no ...
Page 751
momentum to the square of the energy to have the value, M** _(M2+My2+M2\_l(l
+l) jjr —j (16.70) But from (16.60) and (16.65M16.67) the classical result for a
pure (I, m) multipole is U2 U2 w2 (lbJ1) The reason for this difference lies in the ...
momentum to the square of the energy to have the value, M** _(M2+My2+M2\_l(l
+l) jjr —j (16.70) But from (16.60) and (16.65M16.67) the classical result for a
pure (I, m) multipole is U2 U2 w2 (lbJ1) The reason for this difference lies in the ...
Page 758
coefficient, drrk'*2 //+1\1/2 a„a "t)"K2rfl)ll(T^) {Q,+QL) <1693> where the
multipole moments are Qlm = r'Ylpd3x and I (16.94) QU=^y fr'YLVfrxu?) d3x The
moment Qim is seen to be the same in form as the electrostatic multipole moment
qlm ...
coefficient, drrk'*2 //+1\1/2 a„a "t)"K2rfl)ll(T^) {Q,+QL) <1693> where the
multipole moments are Qlm = r'Ylpd3x and I (16.94) QU=^y fr'YLVfrxu?) d3x The
moment Qim is seen to be the same in form as the electrostatic multipole moment
qlm ...
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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