Classical ElectrodynamicsProblems after each chapter |
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Page 392
... particles behave kinematically in the same way , whether charged or neutral . A charged particle can be thought of as a very localized distribution of charge and mass . To find the force acting on such a particle we integrate the ...
... particles behave kinematically in the same way , whether charged or neutral . A charged particle can be thought of as a very localized distribution of charge and mass . To find the force acting on such a particle we integrate the ...
Page 393
... particle : 20120 c2 ( 12.5 ) 0 ) the scalar product ( 12.5 ) gives the ( p ⋅ p ) = ( p ' · p ' ) = In the rest frame of the particle ( p ' energy of the particle at rest : = E ' = 2 ( 12.6 ) To determine & we consider the Lorentz ...
... particle : 20120 c2 ( 12.5 ) 0 ) the scalar product ( 12.5 ) gives the ( p ⋅ p ) = ( p ' · p ' ) = In the rest frame of the particle ( p ' energy of the particle at rest : = E ' = 2 ( 12.6 ) To determine & we consider the Lorentz ...
Page 520
... particle " and a " struck system . " The perturbing fields of the incident particle are replaced by an equivalent pulse of radiation which is analyzed into a frequency spectrum of virtual quanta . Then the effects of the quanta ( either ...
... particle " and a " struck system . " The perturbing fields of the incident particle are replaced by an equivalent pulse of radiation which is analyzed into a frequency spectrum of virtual quanta . Then the effects of the quanta ( either ...
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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