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Page 172
... moving circuit is * d dt s B⚫nda = S дв s at • n da + - $ ( B x v ) • dl ( 6.5 ) Equation ( 6.4 ) can now be written in the form , [ E ' - k ( v × B ) ] • dl = - дв s at • n da ( 6.6 ) This is an equivalent statement of Faraday's law ...
... moving circuit is * d dt s B⚫nda = S дв s at • n da + - $ ( B x v ) • dl ( 6.5 ) Equation ( 6.4 ) can now be written in the form , [ E ' - k ( v × B ) ] • dl = - дв s at • n da ( 6.6 ) This is an equivalent statement of Faraday's law ...
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 no ...
... 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 no ...
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 Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ