Triadic Koch Curve Two antenna forms based on the Triadic Koch Curve will be analyzed. The first a mono/dipole form and the second a loop form. The object of this study is to observe the resonant behavior of an antenna structure that is built up incrementally in sections of four wires. These cyclic elements (much in the sense of array or yagi elements) have an unique shape that is a fundamental pattern for the entire structure. For the Triadic Koch Curve, these 4 wires give the appearance of a triangular jog in a vertical line. The antenna shown consists of 64 straight wires, each 1.1 meter long; total height is 30 meters. This antenna lies entirely within the YZ plane. The basic curve of the greater structure can be found in the first four wires' shape (cyclic element shown in small inset). SWR frequency sweeps were performed on the structure each time a cyclic element was added. The number of resonances were noted and then another cyclic element added. For the structure shown here, there are 16 cyclic elements. In the study of SWR for element 1, there was only 1 resonance between 5 and 50 MHz. When cyclic element 2 (wires 4 through 8) was added, the number of resonances between 5 and 50 MHz increased to 3. With the addition of each additional cyclic element, additional resonances were added to the structure. Fractal Resonances More kinks means more resonances, especially for the Triadic Koch. Through the progressions of constructing this final form, each iteration presented more resonances to a constant frequency sweep of the structure. This SWR chart is for the aggregate of 14 cyclic elements. Mentioned earlier was that for 2 cyclic elements there are 3 resonances. Here for 14 cyclic elements there are something like 18 resonances. An observation of resonance count: There is one resonance for each cyclic element in the structure (over a frequency range of 0 to 2 times the resonance frequency of one cyclic element) Please note this is only observed in the monopole driven form. Same data viewed from a Hi Z perspective of 200 Ohms Folded Koch Curve to present a Loop Here, the curve from above is folded back on itself and fed at the sharp apex in the lower left corner (the junction of wire 1 and wire 64). There are no shorts in the structure as might be suggested by the proximity of points illustrated below. The first difference between this form and the standard form is found in the lower count of resonances for constant wire length. The structure's symmetry lends it self to a number of possible drive points. The first is already described and shown. Another possible site moves the source to the right lower corner, the broad apex. There are also a number of closely paired but mirrored oppositions in the design that could serve as drive points. They lie along the diagonal line extending from the lower left corner to the upper right corner. One such site I evaluated is in the pinch that just precedes the ballooning of the structure (wire 8 end 2 to wire 57 end 1). The intent was to see if the minor loop developed to the left of the drive would serve as a shunting stub to the major loop to the right. Wire 1/64 Fed (as shown above) Note how the number of resonances has dropped by roughly half. That is, it exhibits the number of resonances as found in an 8 element monopole. More notable are the following variations in drive that reduce the number of resonances further. Wire 15 Fed (broad apex with wide symmetry) This feed seems to exhibit a boundary condition. In other data not shown here are similar displays of nulls paired closely in frequency and certainly not harmonically related. The fourth, fifth, and possible sixth nulls show closely paired resonances. Shunt Fed This is an opportunistic feed of the structure found at the pinching of the loop at its closest points. The antenna was fed as two loops in parallel electrically but in series geometrically (W8E2 to W57E1). This method of feed presents roughly the same number of resonances as found in a monopole fractal of 6 cyclic elements. This too exhibits the pairing of resonances such as the sixth and seventh nulls in this display. The Object of this study, to observe tuned shunts, is lost in the resonances as it is. It would be tempting to embrace the twining of resonances at nulls 6 and 7, but these twinnings are too common otherwise.