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 288
... electrons per unit volume in the medium . The damping constant yo / fo can be determined empirically from ... electrons are actually valence electrons of the isolated atoms that become quasi - free and move relatively unimpeded through ...
... electrons per unit volume in the medium . The damping constant yo / fo can be determined empirically from ... electrons are actually valence electrons of the isolated atoms that become quasi - free and move relatively unimpeded through ...
Page 496
... electrons with a uniform background of positive charge . On a very small scale of length we must describe the behavior in terms of a succession of very many two - body Coulomb collisions . But on a larger scale the electrons tend to ...
... electrons with a uniform background of positive charge . On a very small scale of length we must describe the behavior in terms of a succession of very many two - body Coulomb collisions . But on a larger scale the electrons tend to ...
Page 618
... electrons and nuclei . If the particle is heavier than an electron ( mu or pi meson , K meson , proton , etc. ) , the collisions with electrons and with nuclei have different consequences . The light electrons can take up appreciable ...
... electrons and nuclei . If the particle is heavier than an electron ( mu or pi meson , K meson , proton , etc. ) , the collisions with electrons and with nuclei have different consequences . The light electrons can take up appreciable ...
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