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Radar System Engineering

Radar System Engineering

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142 C-II’ RADAR SYSTEMS [SEC. 57<br />

}Vhen j, < f~, the system as outlined must be modified by placing<br />

infinite-attenuation filters after the second detector. The filters are<br />

designed to remove j, completely, ~vhile leaving all but closely adjacent<br />

frequencies undisturbed. In principle, this is no different from the<br />

infinite-at tenuat ion filters already present to remove the d-c signals due<br />

to clutter. Practically, somewhat more trouble is involved, since zero<br />

frequency filters are stable because neither the frequency nor the filter<br />

tuning can change, while both possibilities are present for frequencies<br />

other than zero. Usually also, either by accident or design, various<br />

harmonics of j, will be present and these also must be filtered out.<br />

This is the first case n-e have encountered of a general and almost<br />

exactl theorem to the effect that any periodic modulation can produce<br />

10,000<br />

Sooo<br />

60Q0<br />

4000<br />

2000<br />

z<br />

:1000<br />

“-k800<br />

~ 600<br />

40Q<br />

200<br />

100 10 20 40 60 100 200 400 1000<br />

rm,xin miles<br />

510.- -Maximum repetition or modulation fmquenry as a function of maximum<br />

unambiguous range.<br />

in the receiver, whether by direct leakage or reflection from stationary<br />

objects, only output signals that have the same periodicity; these output<br />

signals can theref ore be removed by a sequence of infinit e-attenuat ion<br />

filters tuned to frequency zero and to all harmonics of the modulation<br />

frequency.<br />

Finally, we note that this system will handle only one target. If<br />

more are present the precise behavior depends on the type of phase<br />

meter used and the best that can be done is to choose a type that measures<br />

range to that target which gives the most intense reflection.<br />

If the system is required to handle more than one target at a time,<br />

discrimination may be made either on the basis of range or of doppler<br />

frequency. If range is used, more sidebands are called for, and the<br />

1The theoremwould be exact if the carrierfrequency were an integralmultiple<br />

of the modulation frequency. When this is not so, the deviations are of the order<br />

~,/fo or less and are usually negligible.

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