Classical ElectrodynamicsProblems after each chapter |
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Page 182
... transverse part , J = J1 + J1 Jt where V x J1 = 0 and V. J1 = O , then the parts can be written ( 6.48 ) = J1 = Jt ... transverse current ( 6.50 ) : V2A - 102A c2 at 2 4πT = - J1 с This is , of course , the origin of the name ...
... transverse part , J = J1 + J1 Jt where V x J1 = 0 and V. J1 = O , then the parts can be written ( 6.48 ) = J1 = Jt ... transverse current ( 6.50 ) : V2A - 102A c2 at 2 4πT = - J1 с This is , of course , the origin of the name ...
Page 243
... Transverse Magnetic and Transverse Electric , respectively , corresponding to specification of the axial com- ponent of the field . In addition to these two types of fields there is a degenerate mode , called the Transverse ...
... Transverse Magnetic and Transverse Electric , respectively , corresponding to specification of the axial com- ponent of the field . In addition to these two types of fields there is a degenerate mode , called the Transverse ...
Page 639
... 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 ...
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Common terms and phrases
4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ