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Radar System Engineering

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SEC.K3.121 RANGE AND HEIGIiT INDICES; SYNCHRONIZATION 521<br />

spaced markers desired.’ Lower-frequency markers are provided by<br />

scaling circuits. A final scaling circuit provides pulses of proper frequency<br />

for triggering the modulator, the sweeps, etc. In the figure it is assumed<br />

that the desired frequency values are successively integral multiples of<br />

the lowest frequent y. If this is not the case, multiple counting channels<br />

are necessary; for simplicity an integral relationship is usually chosen.<br />

When synchronization is external, the oscillator must be shockexcited.<br />

Figure 13.38 illustrates an LC-oscillator widely used in mediumprecision<br />

applications. When VI is conducting, the circuit is quiescent<br />

and energy is stored in the inductance by virtue of the cathode current.<br />

~ Scaling ~ Scaling<br />

Oscillator : Amplifier L :::.;’;.: circuit T circuit<br />

-nl<br />

T nz<br />

I I<br />

I ~-xkw<br />

a. Sinusoid<br />

b<br />

Square wave<br />

c. l-mile marks I I I I I I I I I I I I 1 [ I<br />

c. l-mile marks<br />

(compressed scale) ~11111 — .—— —.— ___ ___<br />

Iulllulllllll<br />

d. 5.mile marks 11111111111111111111 [11111111 11111<br />

e. 20.mile m~ks I I I I I 1 I 1<br />

f Trigger I I<br />

FIG. 13 37,—Derivation of pulses from c-w oscillator.<br />

Interruption of this current by the square wave shock-excites the oscillating<br />

circuit. The resulting voltage wave has an initial phase of zero<br />

and an approximate amplitude of 1-. The constants of the<br />

Hartley circuit of Vj are so chosen that this initial amplitude is just<br />

preserved. In the present example the amplification necessary to produce<br />

steep wave fronts is provided by the regenerative amplifier formed<br />

by VS, V,. Each time that V, is turned on, the surge of current through<br />

its plate circuitz triggers the single-stroke blocking oscillator formed by<br />

V5, giving rise to the desired pulse. It should be noted that a slight<br />

delay is inherent in the production of the first pulse, since a short but<br />

finite time is required to turn on Vq. Later pulses are all displaced by<br />

1For example, in the case of 1-mile markers this frequency is 93.12kc/see.<br />

* The current necessary to charge C? increasesthe positiveness of this action.

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