Reflection, Transmission and Radiation of an EM Surface Wave Incident on a Transition of Surface Reactance |
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Page 25
... waveguides . Theories for transmission lines are well developed , especially when the losses due to radiation or dielectric heat losses are small [ 34 ] . However design theories are lacking in the case of open waveguides , so cut - and ...
... waveguides . Theories for transmission lines are well developed , especially when the losses due to radiation or dielectric heat losses are small [ 34 ] . However design theories are lacking in the case of open waveguides , so cut - and ...
Page 103
... wave radiation from a nonuniform segment of an impedance surface , ' [ 11 ] [ 12 ] [ 13 ] [ 14 ] [ 15 ] [ 16 ] [ 17 ] [ 18 ] ... Open Waveguides , The Golem Press , Boulder , 1971 . S. H. Cho and R. J. King , " Radiation from a finite ...
... wave radiation from a nonuniform segment of an impedance surface , ' [ 11 ] [ 12 ] [ 13 ] [ 14 ] [ 15 ] [ 16 ] [ 17 ] [ 18 ] ... Open Waveguides , The Golem Press , Boulder , 1971 . S. H. Cho and R. J. King , " Radiation from a finite ...
Common terms and phrases
abrupt transition amplitude analytic approximately beam direction Beamwidth capacitive compensation theorem complex reflection coefficient constant CONTINUE RETURN END cose DIMENSION DOUBLE PRECISION Electromagnetic evaluated exponential Fredholm integral equation G₂ GO TO 50 Green's theorem groundwave H₁₂ Hankel function impedance plane impedance profile incident surface wave inductive Irikov jk 1+x² Kay's L₁ line source linear taper M₂ magnetic field nonlinear regression nonuniform surface numerical results numerical solution obtained perfect conductor perturbed fields Phase delay Power balance psine R. J. King radiation field radiation pattern reactive surface reflected surface wave reflection coefficient shown in Fig sine solved SUBROUTINE surface impedance surface reactance surface wave antennas Surface Wave Incident surface wave propagating T₁ T₂ taper length taper T1T2 tion TM surface wave transition region transmission coefficient transmitted surface wave wave propagation X_(x x-xp X₂ XLHA zero ωε Κ