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 536
vector operator. From (11.72) it follows that differentiation with respect to a
covariant component gives a contravariant vector operator. We therefore employ
the notation, (11.76) The 4divergence of a 4vector A is the invariant, daAa =
daA' ...
vector operator. From (11.72) it follows that differentiation with respect to a
covariant component gives a contravariant vector operator. We therefore employ
the notation, (11.76) The 4divergence of a 4vector A is the invariant, daAa =
daA' ...
Page 549
From the discussion at the end of Section 11.6 and especially (11.77) it is natural
to postulate that p and J together form a 4vector J": J° = (cp,J) (11.128) Then the
continuity equation (11.127) takes the obviously covariant form, dar = 0 (11.129)
...
From the discussion at the end of Section 11.6 and especially (11.77) it is natural
to postulate that p and J together form a 4vector J": J° = (cp,J) (11.128) Then the
continuity equation (11.127) takes the obviously covariant form, dar = 0 (11.129)
...
Page 793
integrals at fixed time of the form (17.35) can represent properly the conserved
energymomentum 4vector. Poincar6's solution has some virtues, but it has
deficiencies, too. It requires unknown Poincare stresses in order to provide
stability.
integrals at fixed time of the form (17.35) can represent properly the conserved
energymomentum 4vector. Poincar6's solution has some virtues, but it has
deficiencies, too. It requires unknown Poincare stresses in order to provide
stability.
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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