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 43
1.10 Formal Solution of Electrostatic BoundaryValue Problem with Green
Function The solution of the Poisson or Laplace equation in a finite volume V with
either Dirichlet or Neumann boundary conditions on the bounding surface S can
be ...
1.10 Formal Solution of Electrostatic BoundaryValue Problem with Green
Function The solution of the Poisson or Laplace equation in a finite volume V with
either Dirichlet or Neumann boundary conditions on the bounding surface S can
be ...
Page 225
need to construct the corresponding timedependent Green functions that satisfy (
v,2p Jtf)Gl±\x, V, *, f) — 4ir 8(»«0 80  «0 (6.63) Using (6.56) we see that the
source term for (6.57) is 4TrS(xx')eu"' The solutions are therefore Gi*)(R)«h^.
need to construct the corresponding timedependent Green functions that satisfy (
v,2p Jtf)Gl±\x, V, *, f) — 4ir 8(»«0 80  «0 (6.63) Using (6.56) we see that the
source term for (6.57) is 4TrS(xx')eu"' The solutions are therefore Gi*)(R)«h^.
Page 610
For z0>0, the integral over k0 is f e~'k°xo / e~aVo \ t dkok^=2iriReS(k^) = sin (kzo
) □ The Green function (12.129) is then rw.A_g(zo) f .3. .» .sin (kz0) The
integration over the angles of k leads to Dr(z)=m^ f dK sin («R) sin (kz0) (12.130)
K Jo ...
For z0>0, the integral over k0 is f e~'k°xo / e~aVo \ t dkok^=2iriReS(k^) = sin (kzo
) □ The Green function (12.129) is then rw.A_g(zo) f .3. .» .sin (kz0) The
integration over the angles of k leads to Dr(z)=m^ f dK sin («R) sin (kz0) (12.130)
K Jo ...
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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