Classical ElectrodynamicsProblems after each chapter |
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Page 185
... writing ( w + ie ) in place of w in ( 6.59 ) . Then the Green's function is given by 1 G ( x , t ; x ' , 1 ... written ∞ 1 · G = dx ( e1 [ r− ( R / c ) ] x — ei [ r + ( R / c ) ] x ) 2πRJ -0 ( 6.63 ) From ( 2.52 ) we see that ...
... writing ( w + ie ) in place of w in ( 6.59 ) . Then the Green's function is given by 1 G ( x , t ; x ' , 1 ... written ∞ 1 · G = dx ( e1 [ r− ( R / c ) ] x — ei [ r + ( R / c ) ] x ) 2πRJ -0 ( 6.63 ) From ( 2.52 ) we see that ...
Page 384
... written as a force per unit volume ( representing the rate of change of mechanical momentum of the sources per unit volume ) : f = pE + - J x B J × B 1 / C ( 11.126 ) where J and p are the current and charge densities . Writing out a ...
... written as a force per unit volume ( representing the rate of change of mechanical momentum of the sources per unit volume ) : f = pE + - J x B J × B 1 / C ( 11.126 ) where J and p are the current and charge densities . Writing out a ...
Page 385
... written in the form : этну ( 11.133 ) fu = · θαν με The tensor T , can be written out explicitly in terms of the fields using ( 11.132 ) : Tu T12 T13 -icgi T21 T22 T23 -icge ( 11.134 ) -icg3 ( Tuv ) = T31 T32 T33 -icg1 -icg2 -icg3 น ...
... written in the form : этну ( 11.133 ) fu = · θαν με The tensor T , can be written out explicitly in terms of the fields using ( 11.132 ) : Tu T12 T13 -icgi T21 T22 T23 -icge ( 11.134 ) -icg3 ( Tuv ) = T31 T32 T33 -icg1 -icg2 -icg3 น ...
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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