Classical Electrodynamics |
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Page 182
... transverse part , J = J2 + J1 where V × J1 = O and V. J = O , then the parts can be written ( 6.48 ) = Jt = = - 1 ... transverse current ( 6.50 ) : V2A - 102A c2 12 4πT = - Jt с This is , of course , the origin of the name " transverse ...
... transverse part , J = J2 + J1 where V × J1 = O and V. J = O , then the parts can be written ( 6.48 ) = Jt = = - 1 ... transverse current ( 6.50 ) : V2A - 102A c2 12 4πT = - Jt с This is , of course , the origin of the name " transverse ...
Page 243
... TRANSVERSE MAGNETIC ( TM ) The boundary condition is B1 = 0 everywhere E , │s = 0 = 0 TRANSVERSE ELECTRIC ( TE ) The boundary condition is E. 0 everywhere дв = = 0 an s The designations " Electric ( or E ) Waves " and " Magnetic ( or H ) ...
... TRANSVERSE MAGNETIC ( TM ) The boundary condition is B1 = 0 everywhere E , │s = 0 = 0 TRANSVERSE ELECTRIC ( TE ) The boundary condition is E. 0 everywhere дв = = 0 an s The designations " Electric ( or E ) Waves " and " Magnetic ( or H ) ...
Page 382
... transverse electric field E1 as ẞ - > 1. Even at nonrelativistic velocities where y 1 , this magnetic induction is equivalent to B с q v x r 7.3 ( 11.119 ) which is just the Ampère - Biot - Savart expression for the magnetic field of a ...
... transverse electric field E1 as ẞ - > 1. Even at nonrelativistic velocities where y 1 , this magnetic induction is equivalent to B с q v x r 7.3 ( 11.119 ) which is just the Ampère - Biot - Savart expression for the magnetic field of a ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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