theres no gamma on the open sleeve antenna eddie,
what i think cox means is,
you have two sets of currents, antenna mode and transmission-line mode,
how much current flows in each mode is determined by the impedances Za & Zt which determine currents Ia & It flowing in the antenna,
total current flowing into the antenna is Ia + It,
he talks about it everywhere in the article,
"However, at the resonant frequency of the
sleeves, the impedance of the central monopole
is that of an end fed half-wave monopole and is
very high. Therefore IAis small. If proper element diameters and spacings have been used to
match the transmission line mode impedance,
ZT, to 52 Ω; then IT, the transmission line mode current, is high compared to IA"
if that's not how you read the article eddie please explain your how your single current idea fits in with what is claimed.
can you explain this claim using your single current total cancellation equation eddie ?
"At length ratios approaching 3:1, the antenna mode and transmission line mode impedance become
nearly equal again, and the central monopole again carries a significant portion of the antenna current. The radiation from the top 1/2 λcombines constructively with the radiation from the 1/4-λsleeve elements to
produce gains of up to 3 dB more than just a quarter-wave vertical element alone."
where did cox go wrong eddie ?
did he misunderstand H. B. Barkley who in his paper ( H. B. Barkley, The Open-Sleeve As A Broadband Antenna ) gives a more detailed explanation of the antenna,
reminded me of what cebik told me when he says
"The problem here is somewhat more complex, however, since the effective termination of the transmission line mode is not immediately obvious and the division of the antenna
mode currents is difficult to determine theoretically."
i almost had a shockwave arriving on wwrf moment when i read this eddie
"One method of increasing the resistive term of each transmission line is to increase the effective resistive end loading or radiation losses, by a greater parasite spacing.
This greater spacing has a detrimental effect on the reactance term, but the resistance can predominate for spacings greater than a certain minimum (as it apparently did in the theoretical curve) There is a maximum limit to the spacing usable., above which the low frequency behavior suffers, or severe pattern distortion occurs.
An alternative method may be to flare the parasites outward from the dipole, increasing the losses of the transmission line mode by radiation.
This, of course, is essentially reverting to the idea of the gradual taper to free space as a means of achieving broadbanding but the explana tion of the resistive loading of the transmission lines originates the suggestion.
However, the taper appears to destroy the analogy to the antenna mode of operation, so that analysis by the present theory would be questionable, and the results of this technique would most readily be determined experimentally,
One further means of increasing losses is by a reduction of parasite diameter, but some intrinsic broadbanding effect would undoubtedly be lost."
do skinny flared radials around a fat central monopole remind you of anything eddie ?