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 25
... macroscopic electrical phenomena , as did virtually all other aspects of electromagnetism . The extension of these macroscopic laws , even for charges and currents in vacuum , to the microscopic domain was for the most part an ...
... macroscopic electrical phenomena , as did virtually all other aspects of electromagnetism . The extension of these macroscopic laws , even for charges and currents in vacuum , to the microscopic domain was for the most part an ...
Page 144
... macroscopic quantities . The first observation is that when an averaging is made of the homogeneous equation , V × Emicro = 0 , the same equation , namely , VXE = 0 ( 4.27 ) holds for the averaged , that is , the macroscopic , electric ...
... macroscopic quantities . The first observation is that when an averaging is made of the homogeneous equation , V × Emicro = 0 , the same equation , namely , VXE = 0 ( 4.27 ) holds for the averaged , that is , the macroscopic , electric ...
Page 187
... macroscopic problems this is often not true . The atoms in matter have electrons that give rise to effective atomic currents the current density of which is a rapidly fluctuating quantity . Only its average over a macroscopic volume is ...
... macroscopic problems this is often not true . The atoms in matter have electrons that give rise to effective atomic currents the current density of which is a rapidly fluctuating quantity . Only its average over a macroscopic volume is ...
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 V₁ vanishes vector potential velocity volume wave guide wave number wavelength written zero ΦΩ