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Radar System Engineering

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SEC.5.10] ALTERNATIVE F-M RANGING SYSTEM 149<br />

This ratio depends on target speed, wavelength, repetition rate, and<br />

range accuracy, and might conceivably have almost any value. But in<br />

many cases the value will be too large for this system to be useful,<br />

Specifically, the maximum beat frequency may be written as fr(r/6r) so<br />

that, for example, 1 per cent range accuracy and f, = 10 cps gives<br />

~~ = 1000 CPS, wfich may be compared with a doppler frequency of<br />

894 cps for 10 cm and 100 mph.<br />

6.10. Alternative F-m Ranging <strong>System</strong> .—Another scheme of the<br />

f-m type which is designed to work on multiple targets and in the presence<br />

of clutter may be understood by reference to Fig. 514. This shows, in<br />

the full curve; a sinusoidal dependence<br />

of the transmitted frequency<br />

on time. The total frequency<br />

swing is made large compared to<br />

the doppler frequency. The received<br />

frequency, indicated by the<br />

dotted line, is a similar curve but<br />

(a) displaced to the right by time<br />

delay resulting from transmission<br />

to the target and back and (b) displaced<br />

vertically by doppler shift.<br />

If now the difference between the<br />

transmitted and received frequencies<br />

is passed through a low-pass<br />

filter whose pass band includes frequencies<br />

as high as the maximum<br />

doppler frequency, there will, in<br />

general, be little signal output because<br />

the difference frequency will<br />

be greater than the doppler frequency<br />

over the majority of the<br />

I<br />

FIG. 5.14.—The full curve in the upper<br />

graph shows the instantaneoustransmitter<br />

frequency as a function of time; the dotted<br />

curve shows the received signal; and the<br />

dashed curve, the beat between the two.<br />

The lower curve showsthe same quantities<br />

when 2r/c = nf,, in which case the beat<br />

frequency is constant at the doppler value.<br />

modulation cycle. If, however, the modulation frequency is adjusted<br />

so that one cycle corresponds to the transmission delay time, the difference<br />

frequency will always just equal the doppler frequent y and so a<br />

large output signal will result. Thus, as the modulation frequency is<br />

varied, output occurs whenever n/f, = 2r/c with n any integer and r<br />

the distance to a target. Ground clutter, having no doppler shift,<br />

gives an output that is periodic with period corresponding to the modulation<br />

frequency. The d-c component is easily removed and, if fD < jr,<br />

the other components are removed by the low-pass filter, which passes<br />

only up to f.. If, therefore, f. < j, ground clutter may, in principle,<br />

be removed.<br />

A variant of this scheme turns the receiver off during one modulation

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