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 192
... Scalar Potential If the current density vanishes in some finite region of space , the second equation in ( 5.90 ) becomes VxH = 0 . This implies that we can introduce a magnetic scalar potential Þм such that M H = -VQM ( 5.93 ) just as ...
... Scalar Potential If the current density vanishes in some finite region of space , the second equation in ( 5.90 ) becomes VxH = 0 . This implies that we can introduce a magnetic scalar potential Þм such that M H = -VQM ( 5.93 ) just as ...
Page 219
... the Maxwell equations . Then the inhomogeneous equations in ( 6.28 ) can be written in terms of the potentials as 1 a Sect . 6.4 Time - Varying Fields , Maxwell Equations , Conservation Laws 219 Vector and Scalar Potentials.
... the Maxwell equations . Then the inhomogeneous equations in ( 6.28 ) can be written in terms of the potentials as 1 a Sect . 6.4 Time - Varying Fields , Maxwell Equations , Conservation Laws 219 Vector and Scalar Potentials.
Page 593
... scalar potentials , A and . The appropriate interaction Lagrangian was given by ( 12.8 ) . If we now consider the ... potential energy , LNR NR = _9192 r 12 ( 12.77 ) If attention is directed to the first particle , this can be viewed as the ...
... scalar potentials , A and . The appropriate interaction Lagrangian was given by ( 12.8 ) . If we now consider the ... potential energy , LNR NR = _9192 r 12 ( 12.77 ) If attention is directed to the first particle , this can be viewed as the ...
Contents
L2 The Inverse Square Law or the Mass of the Photon | 1 |
BoundaryValue Problems | 54 |
Multipoles Electrostatics | 136 |
Copyright | |
17 other sections not shown
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4-vector Ampère's law amplitude angle angular distribution angular momentum approximation atomic axis behavior boundary conditions calculate Chapter charge density charge q charged particle classical coefficients collision components conducting conductor consider coordinates cross section current density cylinder d³x defined dielectric constant diffraction dimensions dipole direction discussed electric and magnetic electric field electromagnetic fields electrons electrostatic expansion expression factor force frame frequency given Green function incident integral limit linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic monopole magnitude Maxwell equations medium modes molecules motion multipole multipole expansion multipole moments nonrelativistic normal obtained oscillations parallel parameter photon Phys plane wave plasma polarization problem propagation quantum quantum-mechanical radiation radius region relativistic result scattering shown in Fig sin² solution spectrum sphere spherical surface tensor theorem transverse unit V₁ vanishes vector potential velocity volume wave guide wave number wavelength written zero ΦΩ