Classical ElectrodynamicsProblems after each chapter |
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Page 192
... momentum through the dielectric constant and permeability . ( See also Problem 6.8 . ) With ( 6.90 ) substituted into ( 6.89 ) the integrand becomes 1 1 ДЕ PE + JX B = E ( V.E ) + Bx - BX ( V x B ) ( 6.91 ) 4π at Y Then writing ДЕ a дв ...
... momentum through the dielectric constant and permeability . ( See also Problem 6.8 . ) With ( 6.90 ) substituted into ( 6.89 ) the integrand becomes 1 1 ДЕ PE + JX B = E ( V.E ) + Bx - BX ( V x B ) ( 6.91 ) 4π at Y Then writing ДЕ a дв ...
Page 392
... momentum under Lorentz transformations . For neutral particles with no detectable electromagnetic interactions it is ... momentum and energy of the particle , just as in Section 11.11 . Thus P4 dr . - ff . dx dPu dt = ( 12.2 ) where we ...
... momentum under Lorentz transformations . For neutral particles with no detectable electromagnetic interactions it is ... momentum and energy of the particle , just as in Section 11.11 . Thus P4 dr . - ff . dx dPu dt = ( 12.2 ) where we ...
Page 585
... momentum plus electromagnetic momentum in a given volume vanishes , provided there is no flow of momentum out of or into the volume . Abraham and Lorentz proposed that the apparently mechanical momentum of a charged particle is actually ...
... momentum plus electromagnetic momentum in a given volume vanishes , provided there is no flow of momentum out of or into the volume . Abraham and Lorentz proposed that the apparently mechanical momentum of a charged particle is actually ...
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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