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Radar System Engineering

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656 MOVING-TARGET INDICATION [SEC.16.12<br />

depression angles; some other method must be used, such as the noncoherent<br />

method now to be described.<br />

16.12. The Noncoherent Method. -We have already seen in Fig.<br />

1619 that a target moving in the clutter produces a resultant echo that<br />

varies in both amplitude and phase. To detect the amplitude variations,<br />

all that is required is a receiver that does not limit—that is, one with a<br />

linear-logarithmic response. Since no coherent reference oscillator is<br />

used, this is called the noncoherent method of detecting moving targets.<br />

The ground clutter itself acts as the reference signal,<br />

Modulator Transmitter TR<br />

I<br />

r<br />

Mixer<br />

1<br />

Stable local<br />

oscillator<br />

Signals<br />

I<br />

Mixer<br />

Coherent Phase shift Reference<br />

oscillator<br />

unit<br />

signal<br />

(a)<br />

Receiver<br />

t<br />

Reference signal j, f.+ fd ~c+~d_Phase.shifted<br />

Mixer<br />

Filter<br />

from coherent<br />

fc-f,<br />

reference signal<br />

oscillator<br />

f.hDoppler<br />

frequency<br />

oscillator<br />

(b)<br />

FIG. 16.25 .—MTI on a moving system. (a) Block diagram of system showing location<br />

of phase-shift unit. (h) Simplified block diagram of phase-shift unit<br />

In the noncoherent method the local oscillator does not have to be<br />

stabilized since phase changes are not to be detected. Ho~\-everj the<br />

transmitter must have the same stability as in the coherent method<br />

because the overlapping ground clutter beats ~vith itself if the transmitter<br />

frequency varies from pulse to pulse. As shown in Table 16.1 the stability<br />

requirement is not at all severe.<br />

Another great advantage of the noncoherent method is that it works<br />

even when the radar set is carried on a moving station. This is because<br />

the set is sensitive only to amplitude fluctuations, whereas the motion of<br />

the station causes mainly phase changes in the received echoes. An<br />

amplitude effect, due to the finite beamwidth, will be discussed later.

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