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 258
attached string, as the line of dipoles or solenoid is called, can then be treated
more or less normally within the framework of conventional electromagnetic
interactions where B = Vx A, etc. From (5.55) we see that the elemental vector
potential ...
attached string, as the line of dipoles or solenoid is called, can then be treated
more or less normally within the framework of conventional electromagnetic
interactions where B = Vx A, etc. From (5.55) we see that the elemental vector
potential ...
Page 393
Then the vector potential is of the form already considered in Chapter 5. The
inverse distance can be expanded using (3.70), with the result, lim A(«) =4 I ^k*1 \
jWr"Yt(6\ <fOdV (9.6) This shows that the near fields are quasistationary,
oscillating ...
Then the vector potential is of the form already considered in Chapter 5. The
inverse distance can be expanded using (3.70), with the result, lim A(«) =4 I ^k*1 \
jWr"Yt(6\ <fOdV (9.6) This shows that the near fields are quasistationary,
oscillating ...
Page 394
Without marshalling the full apparatus of vector multipole fields, described in
Chapter 16, we can abstract enough for our immediate purpose. The key ... Then
the result for the vector potential is of the form of (9.6), but with the replacement, „'!
Without marshalling the full apparatus of vector multipole fields, described in
Chapter 16, we can abstract enough for our immediate purpose. The key ... Then
the result for the vector potential is of the form of (9.6), but with the replacement, „'!
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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