12.02.2014 Views

Radar System Engineering

Radar System Engineering

Radar System Engineering

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

152 C-W RADAR SYSTEMS [SEC.5.11<br />

Now the Fourier resolution of Curve a will contain the repetition<br />

frequency and multiples thereof, whereas Curve b contains f. + nf,<br />

but no multiples off, (unless f~ is a multiple of j,). Thus the first or<br />

“clutter” filter that attenuates j, and multiples thereof, while leaving all<br />

else, will remove all signals due to stationary objects, while leaving those<br />

due to moving objects undisturbed. At<br />

~ULfi<br />

point 2 in Fig. 5.15, therefore, the signals<br />

are like those of Fig. 5’17b, and do not<br />

‘“) ~ Contain thefrequencyjr<br />

The signals are now passed through<br />

l.- 2r/c<br />

a full-wave rectifier, the voltage at Point<br />

(b) ;-~;-m””m<br />

i<br />

3 in Fig. 5.15 being like Fig. 5. 17c.<br />

FI~. 5.16.—Transmitted and received<br />

powers as a function of time.<br />

This curve now contains harmonics<br />

njr ~ mjD.<br />

The various doppler sidebands and most of the noise are now removed<br />

by passage through a filter that passes only j, and its multiples, whereupon<br />

the voltage at Point 4 has a form like that shown in Fig. 5. 17d. Thus<br />

the clutter, the doppler frequency, and much noise have been removed,<br />

while the position of the trai~ing edge<br />

of the pulse, which is a measure of<br />

the range, is undisturbed.<br />

The time delay of the trailing‘+ru-<br />

edge of the wave at d, relative to the<br />

modulating pulse, is now a measure<br />

of target range. This time, or range,<br />

may be displayed on the linear radial<br />

sweep of a PPI tube by differentiating<br />

the voltage and using the result<br />

to intensity-modulate the beam.<br />

A few minor points remain to be<br />

considered. First, the explanation<br />

n n I-1<br />

has assumed that the bandwidth is<br />

large enough to pass square waves<br />

without distortion. Actually, the FIG.5.17.—Curvea showsthe voltage<br />

operation is substantially the same at Point 1(cf. Fig. 5,15)dueto a stationary<br />

target and b showsthat due to a moving<br />

when only a few harmonics of j, are target; the dotted envelope curve correspondsto<br />

the doppler frequency. Curve<br />

passed. Second, the function of the<br />

c is the result of passingb through a fullwave<br />

rectifier, and d is the result of<br />

attenuated square-wave voltage introduced<br />

after Point 1 is to balance filtering c.<br />

out the square-wave voltage due to the d-c component of receiver noise,<br />

as modulated by the gating. Finally, it should be noted that the last<br />

filter can have fairly narrow pass bands, thereby considerably reducing<br />

the noise.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!