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 412
... directions other than the direction of incidence . The exact form of the angular distribution of radiated energy is governed by the coherent superposition of multipoles induced by the incident fields , and will in general depend on the ...
... directions other than the direction of incidence . The exact form of the angular distribution of radiated energy is governed by the coherent superposition of multipoles induced by the incident fields , and will in general depend on the ...
Page 475
... direction . A uniform magnetic field Bo acts in the z direction . The system is infinite in the x and y directions . We will look for a steady - state solution for flow in the x direction in which the various quantities depend only upon ...
... direction . A uniform magnetic field Bo acts in the z direction . The system is infinite in the x and y directions . We will look for a steady - state solution for flow in the x direction in which the various quantities depend only upon ...
Page 705
... direction of the incident particle is known and the direction of the radiation is known , but the deflected particle's direction , and consequently that of Aẞ , are not known . Consequently the plane containing the incident beam direction ...
... direction of the incident particle is known and the direction of the radiation is known , but the deflected particle's direction , and consequently that of Aẞ , are not known . Consequently the plane containing the incident beam direction ...
Contents
L2 The Inverse Square Law or the Mass of the Photon | 1 |
BoundaryValue Problems | 54 |
Multipoles Electrostatics | 136 |
Copyright | |
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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 vanishes vector potential velocity volume wave guide wave number wavelength written zero ΦΩ