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Page 172
... moving circuit is * d ± √ B dt B⚫n da = -S дв n da + ( B x v ) • dl ( 6.5 ) s at Equation ( 6.4 ) can now be written in the form , [ E ' A k ( v k ( v x B ) ] • dl = - -k S дв n da s at ( 6.6 ) This is an equivalent statement of ...
... moving circuit is * d ± √ B dt B⚫n da = -S дв n da + ( B x v ) • dl ( 6.5 ) s at Equation ( 6.4 ) can now be written in the form , [ E ' A k ( v k ( v x B ) ] • dl = - -k S дв n da s at ( 6.6 ) This is an equivalent statement of ...
Page 503
... moving with constant speed v ( but subject to accelerations ) in an arbitrary closed path . Successive charges are separated by a constant small interval A. → Starting with the Liénard - Wiechert fields for each particle , and making ...
... moving with constant speed v ( but subject to accelerations ) in an arbitrary closed path . Successive charges are separated by a constant small interval A. → Starting with the Liénard - Wiechert fields for each particle , and making ...
Page 630
... moving circuit , 172 in differential form , 173 in integral form , 170 Fields , of moving particle , 467 of relativistic particle , equivalence of , to pulse of radiation , 382 , 521 Fields of uniformly moving charge , 381 , 467 Fourier ...
... moving circuit , 172 in differential form , 173 in integral form , 170 Fields , of moving particle , 467 of relativistic particle , equivalence of , to pulse of radiation , 382 , 521 Fields of uniformly moving charge , 381 , 467 Fourier ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ