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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 , 1 ; x ' , 1 ... written - G = BARS dx ( e11− ( R / c ) ] x - ei [ r + ( R / c ) ] x ) - 1 27 ( 6.63 ) From ( 2.52 ) we see that the ...
... writing ( w + ie ) in place of w in ( 6.59 ) . Then the Green's function is given by 1 G ( x , 1 ; x ' , 1 ... written - G = BARS dx ( e11− ( R / c ) ] x - ei [ r + ( R / c ) ] x ) - 1 27 ( 6.63 ) From ( 2.52 ) we see that the ...
Page 192
... written dP mech dt 1 + ( E × B ) ď3x = dt Jy 4πc 1 4πT S - - [ E ( V · E ) — E × ( V × E ) + B ( V · B ) − B × ( V x B ) ] ď3x ( 6.93 ) We may tentatively identify the volume integral on the left as the total electromagnetic momentum ...
... written dP mech dt 1 + ( E × B ) ď3x = dt Jy 4πc 1 4πT S - - [ E ( V · E ) — E × ( V × E ) + B ( V · B ) − B × ( V x B ) ] ď3x ( 6.93 ) We may tentatively identify the volume integral on the left as the total electromagnetic momentum ...
Page 385
... written in the form : этни fu = მ . ( 11.133 ) The tensor T , can be written out explicitly in terms of the fields using με ( 11.132 ) : Tu T12 T13 -icgi T21 T22 T23 -icg2 ( 11.134 ) ( Tua , icg ) = ( Tuv ) = = T31 T32 T33 -icgs -icg1 ...
... written in the form : этни fu = მ . ( 11.133 ) The tensor T , can be written out explicitly in terms of the fields using με ( 11.132 ) : Tu T12 T13 -icgi T21 T22 T23 -icg2 ( 11.134 ) ( Tua , icg ) = ( Tuv ) = = T31 T32 T33 -icgs -icg1 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ