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Page 172
... moving circuit is * d S дв B ⚫n da = ⚫n da + dt Js Equation ( 6.4 ) can now be written in the form , s at + $ ( B ( B x v ) • dl ( 6.5 ) C & дв - [ E ' k ( v x B ) ] • dl = - k n da ( 6.6 ) C S at This is an equivalent statement of ...
... moving circuit is * d S дв B ⚫n da = ⚫n da + dt Js Equation ( 6.4 ) can now be written in the form , s at + $ ( B ( B x v ) • dl ( 6.5 ) C & дв - [ E ' k ( v x B ) ] • dl = - k n da ( 6.6 ) C S at This is an equivalent statement of ...
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... moving with constant speed v ( but subject to accelerations ) in an arbitrary closed path . Successive charges are separated by a constant small interval A. - = constant Starting with the Liénard - Wiechert fields for each particle ...
... moving with constant speed v ( but subject to accelerations ) in an arbitrary closed path . Successive charges are separated by a constant small interval A. - = constant Starting with the Liénard - Wiechert fields for each particle ...
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... 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 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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