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Radar System Engineering

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SEC. 3.10] COMPOUND TARGETS 81<br />

effect on the received power of the variation of illumination for a vertical<br />

rectangular sheet and uses the formula thus obtained as a definition of<br />

cross section.<br />

3.10. Compound Targets Extended through Space.—Targets such as<br />

rain, vegetation, 6’window,’” or the surface of the sea are much more<br />

complicated than the targets considered in the preceding sections. It is,<br />

however, easier to predict and verify certain features of the return from<br />

such targets because the compound targets here considered are composed<br />

of large numbers of independent individual scatterers, and for that<br />

reason statistical considerations can be used in their treatment. The<br />

aim of this statistical treatment is to predict the probability distribution<br />

of the returned power and of the correlat ion of successive measurements<br />

of the return power.<br />

It will be useful to distinguish between compound targets distributed<br />

throughout a volume (rain, “ window”) and those distributed over a<br />

surface (vegetation, waves). In this section the first class is considered,<br />

the second being deferred to Sec. 3.11.<br />

The Rain-echo Problem.—Echoes fmm rain are frequently observed<br />

on microwave radar (Fig. 3012). Under some circumstances, the ability<br />

to map out storm areas by radar may be put to good use. In many<br />

applications, however, the presence on the radar screen of storm echoes<br />

(that is, echoes from rain drops within a storm area) is objectionable for<br />

either of two reasons. (1) A small isolated storm cloud at long range<br />

may be mistaken for a legitimate target; airborne sea-search radar is<br />

especially vulnerable to this kind of confusion. (2) Echoes from a storm<br />

area may mask or confuse the echoes from targets at the same range and<br />

azimuth.<br />

The nuisance of “ rain clutter,” which the latter effect is sometimes<br />

called, is most severe when the radar cross section of the desired target<br />

is small. Other factors that determine the intensity of the rain echo<br />

relative to that of the target echo are the beamwidth, pulse length, and<br />

}ravelength of the radar, the distance to the target, and the number and<br />

size of the water drops in the neighborhood of the target. In the case of<br />

a radar set using a pencil beam or a simple fan beam, these factors enter<br />

the problem as follows:<br />

R’A~<br />

-( )<br />

Average rain-echo intensity = _ CT _ .Voo<br />

Target-echo intensity .1” 2 T’<br />

I CI~~ndo,v “ is the British and most commonly used code nanle for conducting<br />

foil or sheetcut into piecesof sucha sizethat eachpieceresonatesas a dipoleat enemy<br />

radar frequency. When this matermlis dispensedfrom aircraft, large volumes of<br />

space can be filled with it. It falls at a speed of only a few malesper hour, Tbe<br />

strong signalsit returnsso effectively mask the radar signalsfrom aircraft that arc<br />

in tbe midst of a cloud of windowthat severaltons of aluminumusedto he dispensed<br />

(24)

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