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Radar System Engineering

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34 TIIE RADAR EQUATION [Sm. 29<br />

the neighborhood of the minimum. The signal threshold power plotted<br />

in Fig. 2.5 is essentially the signal strength, relative to average noise<br />

power, for\vhich anobserver \rouldidentify thesignal correctly nine out<br />

of ten times. Foramore precise defir,itionof thee~perimental criterion<br />

for threshold signal in these tests, the reader is referred to Vol. 24, Sec.<br />

8.2. Our interest just now is in the position of the minimum of each<br />

curve that is seen to lie near @ = 1.2/7. However, departure from this<br />

+12<br />

+ 10 I<br />

+8<br />

‘6<br />

‘8<br />

/ Y<br />

/ L A“<br />

[\<br />

\<br />

/’<br />

‘ ‘% ~<br />

-10<br />

0.1 0.2 0.4 0.6 0.81.0 2 4 6810 20<br />

I.fbandwithln Mc\sec<br />

FIG. 25.-Signalt hreshold vs. i.f bandwidthforapulse durationof lpsec. The signal<br />

power is measuredin unitsof the noisepower, .Y,, within a band 1 Me/see wide, In these<br />

experimentsthe video bandwidth was 10 Mc/sPc,the signal presentationtime was 3 see,<br />

andthe length of the pulseon the screenof the .L.scopewas 1,7mm.<br />

value by a factor of 2 in either direction increases the minimum discernible<br />

signal power by less than 1 db. The radar designer is inclined to<br />

take advantage of this latitude to set @ somewhat greater than 1.2/7 as<br />

this eases the requirement of accurate frequency control. .A vallle of CB<br />

in the neighborhood of 2/r is typical of present practice; there is some<br />

evidence also from controlled experiments on intensity-modulated indicators<br />

(Vol. 24, Chap. 9) which favors this higher value.<br />

The quantity S/kT@, which has been our primary concern in this<br />

section, can now be rewritten by expressing @ in terms of T. If, for<br />

simplicity, we require @ = 1/7 then S/kT@ becomes S7/k T. The prod-

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