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» <br />TaM* 1 —Propagation Oistanct vartus <br />Radiation Anglo <br />(Data oxtraetad from Fig 3) <br />500 <br />5n»8i.t «*0* 0<lT*».Ct <br />~<M ItMt***' <br />tad <br />tranamitaiaa) tor tfio nomina l rango of virtual ttoighta <br />for tlio f and P2 loyora, and for tha FI layar. <br />Tha sacond important point to ba racognizad in <br />multihop propagation ia that tha trigortomatry of tha first <br />hop ganaraHy astablishas tha trigonometry for all <br />succaading hops. And it is tha radiation angla at the <br />transmitter which sets up tha trigonometry tor tha first <br />hop. Solving a propagation triangle is simplified with tha <br />aid of tha graph in Fig 3.' In this graph the radiation angle <br />in degrees is given on tha left, and tha singla-hop <br />distance foi tha affective layar height along tha bottom. <br />Tabia t shows tha optimum propagation distance tor <br />various radiation anj^. Tha data tor this table was read <br />from the graph of Fig 3. based on an assumed F-layar <br />height of 131 miles. <br />From Table 1. if the radiation angle from a given <br />transmitting antenna is concentrated at 30**. tha first and <br />succaading hops in radio propagation will span about <br />650 miles each. With a usable maximum limit of five hops <br />under the best of conditions, one can protect that <br />the greatest distance tor optimum communications for <br />a 30* wave angle is five times 650 miles, or 3250 miles. <br />For affective communications over greater distances, it <br />would be necessary to lower the radiation angle at the <br />tranamittar antenna site. As will be discussed s.honty, this <br />can ba dona only by increasing the height of tha horn <br />zontal transmitting antenna. <br />Although the discussion in the preceding para* <br />graphs has bean in terms of a transmitting antenna, the <br />same principles apply whan tha antenna is used for <br />recaption. A high antenna will receive low-artgle signals <br />more effactivoly than will a low antenna. The point of <br />these several paragraphs may be summarized briefly: <br />Tha vertical angla of radiation is tha key factor in <br />determining affective communications distances <br />beyond line of sight. <br />fisastion <br />Angie. <br />Dtignn <br />2 <br />4 <br />8 <br />10 <br />IS <br />20 <br />30 <br />40 <br />Optimum <br />PfOppgMon <br />Distanet. Mips <br />22SO <br />2100 <br />1650 <br />1S00 <br />1200 <br />1000 <br />650 <br />450 <br />Scientists and engineers recognize that mode <br />other the" signal hopping account for the propagatic <br />of radio waves over thousands of miles. Howeve <br />studies of actual radio propagation in which the write <br />has participated have dieplayed signals with as many e <br />5 hops, so the hopping mode is one distinct possibility <br />Whatever the propagation mode, there is unanimou <br />agreement that the most effective communications at H <br />most often accompany the lowest radiation angle. <br />Horlaental Antennas <br />A simple antenna that is commonly used for H <br />communications is the horizontal half*wave dipole. Th <br />dipole is a straight length of wire (or tubing) into whic <br />radio-frequency energy is fed at the center. Because i <br />its simplicity, the dip^ may be easily subjected t <br />theoretical performance analyses. Further«4he result <br />of proper analyses are borne out in practice. For thes <br />reasons, the half-wave dipole becomes a convenier <br />performance standard against which other antenn. <br />systems can be compared. The dipole antenna, whe: <br />viewed from one end. radiates an equal amount of powe <br />in all directions. <br />Because the earth acts as a reflector for HF radi <br />waves, the directive properties of any antenna art <br />modified considerably by the earth unMrneath it. if <br />dipole antenna is placed horizontally above the earth <br />most of the energy radiated downward from the dipou <br />is reflected upward The reflected waves combine witr <br />the direct waves (those radiated at angles above th^ <br />honzontal) in various ways, depending on the height o <br />the antenna, the frequency, and the electrical character <br />istics of the ground under and around the antenna. <br />At some vertical angles above tne horizon, the direc <br />and reflected waves may be exactly in phase-~that is <br />the maximum signal or field strengths of both waves arr <br />reached at the same instant at some distant point. In thr. <br />Trom The APRL AnUnna Book, 14th edition. Chapter 1 . Fig 12 <br />>HP baexscatier studies by Raytheon Company under contrac <br />with Rome Air Oevekipment Center. Gnffiss AFB. NY. A par <br />of this study was done at Raytheon's South Dartmouth <br />Mass, field site. Jan*Jun. 1960.