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Page 182
... transverse part , J = J1 + Jt where V x J1 = 0 and V. J = O , then the parts can be written ( 6.48 ) J , Ji = = - 1 ... transverse current ( 6.50 ) : V2A — 102A c2 at 2 4πT = Jt с This is , of course , the origin of the name " transverse ...
... transverse part , J = J1 + Jt where V x J1 = 0 and V. J = O , then the parts can be written ( 6.48 ) J , Ji = = - 1 ... transverse current ( 6.50 ) : V2A — 102A c2 at 2 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 Ez 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 Ez 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
... Transverse magnetic ( TM ) waves , at- tenuation of , in wave guides , 251 connection of , with multipole mo- ments , 553 f . cylindrical , 243 in cylindrical cavity , 254 in dielectric wave guide , 263 spherical , 545 Transverse waves ...
... Transverse magnetic ( TM ) waves , at- tenuation of , in wave guides , 251 connection of , with multipole mo- ments , 553 f . cylindrical , 243 in cylindrical cavity , 254 in dielectric wave guide , 263 spherical , 545 Transverse waves ...
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