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 21
To determine its value, consider the surface integral of the time derivative of D/c
over the open surface identical in shape to C, but moving with the interface at
velocity v and instantaneously coincident with C in Fig. 1.5. The integral is J c dt ...
To determine its value, consider the surface integral of the time derivative of D/c
over the open surface identical in shape to C, but moving with the interface at
velocity v and instantaneously coincident with C in Fig. 1.5. The integral is J c dt ...
Page 141
Thus the integral (4.16) is J<r E(x) d3x = ^f\d3x' ^ n'p(x') (4.17) where (r<, r>) = (r'
, R) or (R, r') depending on which of r' and R is larger. If the sphere of radius R
completely encloses the charge density, as indicated in Fig. 4.1a, then r< = r/ and
...
Thus the integral (4.16) is J<r E(x) d3x = ^f\d3x' ^ n'p(x') (4.17) where (r<, r>) = (r'
, R) or (R, r') depending on which of r' and R is larger. If the sphere of radius R
completely encloses the charge density, as indicated in Fig. 4.1a, then r< = r/ and
...
Page 573
From the first postulate of special relativity the action integral must be a Lorentz
scalar because the equations of motion are determined by the extremum
condition, 8A = 0. If we introduce the particle's proper time t into (12.3) through dt
=ydT, the ...
From the first postulate of special relativity the action integral must be a Lorentz
scalar because the equations of motion are determined by the extremum
condition, 8A = 0. If we introduce the particle's proper time t into (12.3) through dt
=ydT, the ...
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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