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Radar System Engineering

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630 MOVING-TARGET INDICATION [SEC. 162<br />

To obtain range information with the scheme of Fig. 16”4, the phones<br />

can be replaced by an A-scope synchronized with the modulator. The<br />

appearance of the A-scope is shown in Fig. 16”5, where one moving target<br />

C.w f Power<br />

transmitter<br />

amplifier<br />

t<br />

i<br />

‘‘f<br />

I<br />

1’<br />

Pulse<br />

F1m 16,4,—Doppler effect with pulsed system suitable for low frequencies.<br />

is seen among several stationary ones. The butterfly-like appearance<br />

of the moving target is the result of the variation in pulse amplitudes<br />

shown in Fig. 16.4. Stationary targets exhibit constant phase from pulse<br />

to pulse, and therefore a steady<br />

Modulator<br />

amplitude.<br />

The arrangement of Fig. 16.4 ~- —_______<br />

can be used at frequencies of a few<br />

t ‘;F::g TR switch<br />

hundred megacycles per second but ~--—1 -- __,<br />

Reference ,<br />

is not practical at microwave fre- ,<br />

---_l oscillator -__—l<br />

quencies in the absence of suitable L-+—— Receiver<br />

power amplifiers. However, the C-wreference 1<br />

s)gnal<br />

t<br />

A-scope<br />

FIG. 16.5.—Doppler beats on an & FIG. 16.6.—Doppler system for microscope.<br />

waves. Dotted lines show what must<br />

be added to ordinary radar set.<br />

same effect 1 can be obtained by the circuit of Fig. 16.6, which shows the<br />

basic diagram of a microwave pulsed radar, with the addition of a reference<br />

oscillator. This reference oscillator provides a c-w signal with which<br />

to beat the incoming echoes. Since the transmitter starts with random<br />

phase from pulse to pulse, it is necessary to match the phase of the reference<br />

oscillator to that of the transmitter at each transmitted pulse.<br />

1(,second time around~) echoes—signalsreceived from the second preceding<br />

pulse-will not be canceled by the arrangement of Fig. 166.

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