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 186
... magnetic induction . The potential energy of a permanent magnetic moment ( or dipole ) in an external magnetic field can be obtained from either the force ( 5.69 ) or the torque ( 5.71 ) . If we interpret the force as the negative ...
... magnetic induction . The potential energy of a permanent magnetic moment ( or dipole ) in an external magnetic field can be obtained from either the force ( 5.69 ) or the torque ( 5.71 ) . If we interpret the force as the negative ...
Page 204
... magnetic field on the z = 0 * side of the plane in the absence of the hole . Figure 9.4 shows qualitatively how the magnetic field lines distort to give rise to the dipole field . In the opening itself ( z = 0 , 0≤p < a ) the ...
... magnetic field on the z = 0 * side of the plane in the absence of the hole . Figure 9.4 shows qualitatively how the magnetic field lines distort to give rise to the dipole field . In the opening itself ( z = 0 , 0≤p < a ) the ...
Page 266
... magnetic fields between the plates to second order in powers of the frequency ( or wave number ) , neglecting the ... field , and a transverse magnetic field is applied , there develops a component of electric field in the direction ...
... magnetic fields between the plates to second order in powers of the frequency ( or wave number ) , neglecting the ... field , and a transverse magnetic field is applied , there develops a component of electric field in the 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