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Communications Antennas
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Electronics Technician Volume 07-Antennas and Wave Propagation
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Vertical Monopole LPA

Figure  2-12.—Trideco-type  antenna. Figure  2-11.—Goliath-type  antenna. HIGH   FREQUENCY   (HF) LOW  FREQUENCY  (LF) Antennas for lf are not quite as large as antennas for vlf, but they still occupy a large surface area. Two examples  of  If  antenna  design  are  shown  in  figures 2-13  and  2-14.  The  Pan  polar  antenna  (fig.  2-1  3)  is an umbrella top-loaded monopole. It has three loading loops  spaced  120  degrees  apart,  interconnected  between the  tower  guy  cables.  Two  of  the  loops  terminate  at ground, while the other is used as a feed. The NORD antenna  (fig.  2-14),  based  on  the  the  folded-unipole principle, is a vertical tower radiator grounded at the base  and  fed  by  one  or  more  wires  connected  to  the top  of  the  tower.  The  three  top  loading  wires  extend from  the  top  of  the  antenna  at  120-degree  intervals to  three  terminating  towers.  Each  loading  wire  has a length approximately equal to the height of the main tower  plus  100  feet. The  top  loading  wires  are insulated  from  ground  and  their  tower  supports  are one-third  the  height  of  the  transmitting  antenna. High-frequency  (hf)  radio  antenna  systems  are  used to  support  many  different  types  of  circuits,  including ship-to-shore, point-to-point, and   ground-to-air broadcast. These diverse applications require the use of various numbers and types of antennas that we will review  on  the  following  pages. Yagi The Yagi antenna is an end-fired parasitic array. It  is  constructed  of  parallel  and  coplaner  dipole elements  arranged  along  a  line  perpendicular  to  the axis  of  the  dipoles,  as  illustrated  in  figure  2-15.  The most limiting characteristic of the Yagi antenna is its extremely  narrow  bandwidth.  Three  percent  of  the center  frequency  is  considered  to  be  an  acceptable bandwidth  ratio  for  a  Yagi  antenna.  The  width  of the array is determined by the lengths of the elements. The length of each element is approximately one-half 2-7

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