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Radar System Engineering

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260 RADAR BEACONS [SEC. 8.6<br />

lower than that of the radar by a factor of 20 or so. Either the beamwidth<br />

of the antenna for receiving replies from the beacon is made very<br />

broad or this antenna is made omnidirec bional. Microwave angular<br />

discrimination is still provided by the sharpness of the interrogating<br />

beam—again only for beacons at ranges beyond that for which side lobes<br />

begin to cause broadening of the reply. Figure 8.9 shows a whole set of<br />

replies from such a beacon, exposures having been made every few sweeps<br />

of the PPI. The interrogations were at 10 cm, the replies at 1.5 m. The<br />

principal reason for using such a beacon rather than one that gives a<br />

microwave reply is the relative simplicity of the low-frequency transmitter<br />

and antenna of the beaeon. Also, by placing several simple<br />

antennas and receivers for the interrogation at different places on an aircraft,<br />

it is possible to achieve a good approximation to an effectively<br />

omnidirectional pattern for the interrogation link. This is almost<br />

impossible to achieve with single simple microwave antennas because of<br />

interference effects. It is necessary to put the outputs of such multiple<br />

receivers in parallel after detection so that there will not be a combination<br />

of r-f signals in varying phases to give rise to interference maxima and<br />

minima.<br />

The foregoing discussion implies that the broadening of the arcs for<br />

beacon replies is greater than that for radar signals. This is not the case,<br />

however, if the maximum range for both is the same. If G~U and G(,oh)<br />

are the respective gains of the antenna at the center of the pattern and at<br />

the maximum of the first side lobe and R! and R;[l.h) the corresponding<br />

maximum ranges for interrogation of the beacon (to give minimum<br />

triggering power), from Eq. (5) we get GJ(R:) 2 = G(l.~)/R~O.~).<br />

The same line of argument followed through with the radar equation<br />

gives P-J(R:) 4 = G2(]~~)/R&~), which gives the same value of R,(,ok)<br />

when R: is the same. In practice, however, the broadening of the beacon<br />

signals is likely to be greater since i~ is customary and usually desirable<br />

to set the sensitivity of the beacon receiver so that the maximum freespace<br />

range is considerably greater than the radar range to an average<br />

target. This is done partly to ensure increased range and partly to allow<br />

for the considerable unavoidable variations between the receivers of<br />

different beacons as installed and operated.<br />

8.6. Frequency Considerations. General.4ince beacon replies are<br />

much like radar echoes, the considerations involved in choosing the frequency<br />

region for a system in order to get the desired resolution are much<br />

the same. In general, the higher the frequency, the better the azimuth<br />

discrimination for a given tolerable size of antenna system. This<br />

advantage of improved angular separation with increased frequency is<br />

somewhat offset by a tendency toward increased size and weight of transmitters<br />

needed for a given range performance.

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