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07-25-1994 Council Packet
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07-25-1994 Council Packet
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r <br />I <br />fk <br />fI' <br />th <br />r'- <br />r <br />compass dirsctions. as a solid tins. The broken line in <br />Fig 6 showrs the pattern of a haif-waveiength dipole, for <br />comparison. Fig 7 shows the elevation plane or vertical- <br />profile pallem. This pattern is that seen from the ends <br />line again repieaents the Vagi, and the broken line the <br />dipole, that‘‘perfact cede** 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 oflan-used type of becm antenna is the <br />quad array. TypicaNy. a quad is constructed with two or <br />more wire alemama in the form of a square or a diamond. <br />The conducting wires are usuaNy 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 Yagt beam. <br />The vertical patterns of Figs 4 and 5 were calcuiaied <br />by assuming the earth is a pertsct 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 wiN be <br />slightly different, depending upon the electrical con <br />ductivity and dielectnc constant of the soil, and upon the <br />radio frequency. Computer programs are available to <br />take these factors mto account, and reliable relculations <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 He personal <br />computer.* “Average” soil conditions were used for <br />these plots, that is. a conductivity of 5 miHisiemens per <br />meter arKl a dielectric constant of 15.« These patterns <br />compare the performance of Yagi arrays at heights of <br />3$ 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 />tor clarity. Otherwise the multiple lobes become indis <br />tinguishable. <br />commercisHy avaiiabie software program. ANNIE, was used <br />to calcuiaie ail patterns presented m this paper <br />*$uen soil conditions may be considered typical (or the central <br />part of tne United States, such as the Ohio and Mississippi <br />river valleys. <br />•C <br />Fig S—Vertica l profile pattern of a 7-MHz Yagi beam <br />over average earth at a height of 70 feet (solid line) <br />and at 35 feel (broken line). <br />^0 <br />at 70 feel (aoNd haa) and at 38 feat (brekan Nna) <br />Fig 10—Vertical profile patiam of a i4-MHa Vagi beam <br />at 70 feat (solid Hno) and at M foot (broken Kne). <br />Fig 11—Vertical-prefilo pattom of an ig.l-MNz Yagi <br />beam at 70 feet (solid line) and at 35 foot (broken lino). <br />Fig 12—Vortlcai<^rofilo pattern of a 21-MHa Yagi beam <br />at 70 feet (solid line) and at 35 feet (broken line). <br />1
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