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Radar System Engineering

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704 RADAR RELAY @EC. 17.7<br />

illustrates such a method. The stators of the scanner synchro are excited<br />

by equal-amplitude signals of frequencies f, and f,, as are the two equal<br />

primaries of a transformer whose secondary is in series with the synchro<br />

rotor. The voltage across the combination is then<br />

jl(A + B sin 0) + ~@ + B cos o),<br />

where fl and fzrepresent the audi~frequency input voltages and A and B<br />

are constants. Since A is greater than B, the amplitude terms are always<br />

positive. This voltage is mixed with a constant-amplitude a-f signal of<br />

frequency fj (which is used for AGC at the receiver), and the combination<br />

is used to modulate a subcarrier of somewhat higher frequency than the<br />

maximum required for video signals. The modulated carrier, the video<br />

signals, and the trigger pulse are then mixed and passed on to the transmitter<br />

proper. At the receiving station, the various component signals are<br />

separated by appropriate filters, as indicated in Fig. 17.11, and the sine<br />

and cosine signals passed through detectors. The resulting voltages contain<br />

a d-c component of magnitude C (with respect to the detector bias<br />

point) and a varying component of amplitude D, the sum being always<br />

positive. The d-c component can be prevented from affecting the final<br />

device by relating its bias level properly to that of the detector. The<br />

scheme of adding a constant a-f component to the signal is intended to<br />

preserve the phase sense of the components varying sinusoidally with the<br />

scanner rotation; in this case it is considerably simpler than transmitting<br />

a reference signal to be used in keying a phase-sensitive rectifier.<br />

Pulse-timing Methods.—The simplest method of using pulse-timing<br />

techniques to relay sine and cosine information can be understood by<br />

referring to the timing diagram of Fig. 17.12. A basic pulse occurs once<br />

each radar cycle. The delay of a second pulse is varied with respect to it<br />

in accordance with the expression A + B sin O,where A must be greater<br />

than B in order that the delay shall never become negative. A third<br />

pulse is delayed with respect to the “sine” pulse by an amount proportional<br />

to A + B cos 0. In the interpretation of the data it is only necessary<br />

to provide for each function a circuit that will develop a voltage<br />

proportional to the time lapse between the members of a particular pulse<br />

pair.<br />

The essentials of such an equipment are illustrated in Fig. 17.12.<br />

Slowly varying sine and cosine potentials are furnished by a data transmitter<br />

(which can be either a d-c excited sine-cosine potentiometer or a<br />

two-phase synchro whose output signals are rectified in a phase-sensitive<br />

manner). Each of these potentials controls the operation of a linear<br />

delay circuit. The sine delay circuit is triggered by the basic pulse, and<br />

the cosine circuit is triggered by the sine pulse produced by the sine delay<br />

circuit. Each. gives a finite delay A when the controlling voltage is zero

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