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 219
The units employed in writing the Maxwell equations (6.28) are those of the
previous chapters, namely, Gaussian. For the reader more at home in other units,
such as MKSA, Table 2 of the Appendix summarizes essential equations in the ...
The units employed in writing the Maxwell equations (6.28) are those of the
previous chapters, namely, Gaussian. For the reader more at home in other units,
such as MKSA, Table 2 of the Appendix summarizes essential equations in the ...
Page 263
(a) Starting from the expression (5.10) for the force between the loops, show that
it can be written Fu=I,IJVllMia(R) where M12 is the mutual inductance of the loops
, M'j(R)=?ttx7=xTTRi and it is assumed that the orientation of the loops does not ...
(a) Starting from the expression (5.10) for the force between the loops, show that
it can be written Fu=I,IJVllMia(R) where M12 is the mutual inductance of the loops
, M'j(R)=?ttx7=xTTRi and it is assumed that the orientation of the loops does not ...
Page 785
given by the negative of the Larmor power: dE_ 2e2,.,2_ 2e2 {dVY dt~ 3c3W"
3m2c3\dr) While the definition of t (17.3) this can be written S~s(2)' Since the
change in energy is assumed to be small in one cycle of the orbit, the righthand
side ...
given by the negative of the Larmor power: dE_ 2e2,.,2_ 2e2 {dVY dt~ 3c3W"
3m2c3\dr) While the definition of t (17.3) this can be written S~s(2)' Since the
change in energy is assumed to be small in one cycle of the orbit, the righthand
side ...
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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