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06-16-1997 Planning Packet
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06-16-1997 Planning Packet
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compass directions, as a solid line. The broken line in <br />Fig 6 shows the pattern of a half-wavelength dipole, for <br />comparison. Fig 7 shows the elevation plane or vertical- <br />profile pattern. This pattern is that seen from the ends <br />of the elements, with the antenna in free space. The solid <br />line again represents the Yagi. and the broken line the <br />dipole, that "perfect circle" which was mentioned earlier. <br />Performance of most other Yagi-type arrays with three <br />or four elements will not be significantly different from <br />the patterns shown here. <br />Another often-used type of becm antenna is the <br />quad array. Typically, a quad is constructed with two or <br />more wire elements in the form of a square or a diamond. <br />The conducting wires are usually supported by X-shaped <br />frames of wood or fiberglass material. For the same <br />number of elements and spacing, the performance of a <br />quad beam is generally similar to that of a Yagi beam. <br />The vertical patterns of Figs 4 and 5 were calculated <br />by assuming the earth is a perfect reflector, an unrealistic <br />situation. Actual earth does not reflect all of the radio <br />frequency energy striking it; some absorption takes <br />place. Over real earth, therefore, the patterns will be <br />slightly different, depending upon the electrical con <br />ductivity and dielectric constant of the soil, and upon the <br />radio frequency. Computer programs are available to <br />take these factors into account, and raliable calculations <br />of patterns over real earth may be made. Yagi patterns <br />over real earth are shown in Figs 8 through 14. These <br />patterns were calculated with an Apple lie personal <br />computer.3 "Average ” soil conditions were used for <br />these plots, that is. a conductivity of 5 millisiemens per <br />meter and a dielectric constant of 15.< These patterns <br />compare the performance of Yagi arrays at heights of <br />35 and 70 feet. In Figs 8 through 12. the broken line is <br />the plot for a 35-foot height, and the solid line for 70 feet. <br />For 24.9 and 28 MHz. Figs 13 and 14. it is helpful to <br />present the 35- and 70-foot patterns in separate graphs, <br />for clarity. Otherwise the multiple lobes become indis <br />tinguishable. <br />3A commercially available software program. ANNIE, was used <br />to calculate all patterns presented in this paper. <br />‘‘Such soil conditions may be considered typical for the central <br />P3rt of the United States, such as the Ohio and Mississippi <br />river valleys. <br />Fig 8—Vertical-profile pattern of a 7-MHz Yagi beam <br />over average earth at a height of 70 feet (solid line) <br />and at 35 feet (broken line). <br />Fig 9—Vertical-profile pattern of a 10.1 -MHz Yagi beam <br />at 70 feet (solid line) and at 35 feel (broken line). <br />Fig 10 —Vertical-profile pattern of a 14-MHz Yagi beam <br />at 70 feet (solid line) and at 35 feet (broken line). <br />Fig 11 —Vertical-profile pattern of an 18.1-MHz Yagi <br />beam at 70 feet (solid line) and at 35 feet (broken line). <br />Fig 12—Vertical-profile pattern of a 21-MHz Yagi beam <br />at 70 feet (solid line) and at 35 feet (broken line). <br />41
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