Classical ElectrodynamicsProblems after each chapter |
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Page 315
... force equation to the magnetic induction B via Ampère's law and to use the infinite conductivity expression ( 10.9 ) to eliminate E from Faraday's law to yield ( 10.13 ) . The magnetic force term in ( 10.2 ) can now be written ( J x B ) ...
... force equation to the magnetic induction B via Ampère's law and to use the infinite conductivity expression ( 10.9 ) to eliminate E from Faraday's law to yield ( 10.13 ) . The magnetic force term in ( 10.2 ) can now be written ( J x B ) ...
Page 337
... force equation in ( 10.91 ) is independent of magnetic field , we suspect that there exist solutions of a purely electrostatic nature , with B = 0. The continuity and force equations can be combined to yield a wave equation for the ...
... force equation in ( 10.91 ) is independent of magnetic field , we suspect that there exist solutions of a purely electrostatic nature , with B = 0. The continuity and force equations can be combined to yield a wave equation for the ...
Page 384
... force equation and the conservation laws of momentum and energy . The Lorentz force equation can be written as a force per unit volume ( representing the rate of change of mechanical momentum of the sources per unit volume ) : f = pE + ...
... force equation and the conservation laws of momentum and energy . The Lorentz force equation can be written as a force per unit volume ( representing the rate of change of mechanical momentum of the sources per unit volume ) : f = pE + ...
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Common terms and phrases
4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ