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 340
For simplicity, the crosssectional size and shape are assumed constant along
the cylinder axis. With a sinusoidal time dependence c_u°' for the fields inside the
cylinder, the Maxwell equations take the form: VxE=iB VxB = iu,€E r c VB=0, ...
For simplicity, the crosssectional size and shape are assumed constant along
the cylinder axis. With a sinusoidal time dependence c_u°' for the fields inside the
cylinder, the Maxwell equations take the form: VxE=iB VxB = iu,€E r c VB=0, ...
Page 429
one over the screen and its apertures (Si), the other over a surface "at infinity" (S2
). Since the fields in region II are assumed to be transmitted through Si, they are
outgoing waves in the neighborhood of S2. The fields and hence i//(x) will satisfy
...
one over the screen and its apertures (Si), the other over a surface "at infinity" (S2
). Since the fields in region II are assumed to be transmitted through Si, they are
outgoing waves in the neighborhood of S2. The fields and hence i//(x) will satisfy
...
Page 456
Since we have assumed that the observation point is many wavelengths from the
slab, this integral can be neglected. Neglecting the oscillating contribution at the
upper limit R+» (this can be made to vanish somewhat more plausibly by ...
Since we have assumed that the observation point is many wavelengths from the
slab, this integral can be neglected. Neglecting the oscillating contribution at the
upper limit R+» (this can be made to vanish somewhat more plausibly by ...
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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