Classical ElectrodynamicsIntroduction to electrostatics. Boudary-value problems in electrostatics: I. Boundary-value problems in electrostatics: II. Multipoles, electrostatics of macroscopic media, dielectrics. Magnetostatics. Time-varying fields, maxwell equations, conservation laws. Plane electromagnetic waves and wave propagation. Wave guides and resonant cavities. Simple radiating systems, scattering, and diffraction. Magnetohydrodynamics and plasma physics. Special theory of relativity. Dynamics of relativistic particles and electromagnetic fields. Collisions between charged particles, energy loss, and scattering. Radiation by moving charges. Bremsstrahlung, method of virtual quanta, radiative beta processes. Multipole fields. Radiation damping, self-fields of a particle, scattering and absorption of radiation by a bound system. Units and dimensions, basic units and derived units. Electromagnetic units and equations. Various systems of electromagnetic units. Conversion of equations and amounts between Gaussian units and MKSA units. |
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Page 48
... conductors , the linear functional dependence of the potential on the charge density implies that the potential of the ith conductor can be written as V1 = Σ p1Q , ( i = 1 , 2 , ... , n ) where the p1 , depend on the geometry of the ...
... conductors , the linear functional dependence of the potential on the charge density implies that the potential of the ith conductor can be written as V1 = Σ p1Q , ( i = 1 , 2 , ... , n ) where the p1 , depend on the geometry of the ...
Page 335
... Conductor As was mentioned at the end of Section 7.7 , the problem of reflection and refraction of waves at an interface of two conducting media is somewhat complicated . The most ... Conductor Fields at the Surface of and within a Conductor.
... Conductor As was mentioned at the end of Section 7.7 , the problem of reflection and refraction of waves at an interface of two conducting media is somewhat complicated . The most ... Conductor Fields at the Surface of and within a Conductor.
Page 336
... conductor , aside from a thin transitional layer at the surface . If we wish to examine that thin transitional ... conductor there exists only a normal electric field E , and a tangential magnetic field H , as for a perfect conductor ...
... conductor , aside from a thin transitional layer at the surface . If we wish to examine that thin transitional ... conductor there exists only a normal electric field E , and a tangential magnetic field H , as for a perfect conductor ...
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
Common terms and phrases
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 vanishes vector potential velocity volume wave guide wave number wavelength written zero ΦΩ