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Page 182
... transverse part , O , then the parts can be written ( 6.48 ) Ji = - 4πT V ' . J ' Ix - x ' d3x ' Jt = ▽ 4π 1 x V x ... transverse current ( 6.50 ) : V2A — 1 02A c2 at 2 4πT = Jt This is , of course , the origin of the name “ transverse ...
... transverse part , O , then the parts can be written ( 6.48 ) Ji = - 4πT V ' . J ' Ix - x ' d3x ' Jt = ▽ 4π 1 x V x ... transverse current ( 6.50 ) : V2A — 1 02A c2 at 2 4πT = Jt This is , of course , the origin of the name “ transverse ...
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 ...
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