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 165
(b) If it is known that Q = 2x 10~24 cm2 and that W/h is 10 MHz, where h is
Planck's constant, calculate (dEJBz)0 in units of ... □••8 A very long, right circular,
cylindrical shell of dielectric constant 6 and inner and outer radii a and b,
respectively, ...
(b) If it is known that Q = 2x 10~24 cm2 and that W/h is 10 MHz, where h is
Planck's constant, calculate (dEJBz)0 in units of ... □••8 A very long, right circular,
cylindrical shell of dielectric constant 6 and inner and outer radii a and b,
respectively, ...
Page 166
4.10 Two concentric conducting spheres of inner and outer radii a and b,
respectively, carry charges ħQ. The empty space between the spheres is half
filled by a hemispherical shell of dielectric (of dielectric constant e), as shown in
the figure.
4.10 Two concentric conducting spheres of inner and outer radii a and b,
respectively, carry charges ħQ. The empty space between the spheres is half
filled by a hemispherical shell of dielectric (of dielectric constant e), as shown in
the figure.
Page 296
7.7 Waves in a Conducting or Dissipative Medium We have seen in Section 7.5
that the dielectric constant of a medium is generally complex, whether the
material is an insulator or conductor. For insulators the imaginary part of e can be
...
7.7 Waves in a Conducting or Dissipative Medium We have seen in Section 7.5
that the dielectric constant of a medium is generally complex, whether the
material is an insulator or conductor. For insulators the imaginary part of e can be
...
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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