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Radar System Engineering

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510 THE RECEIVING S YSTEhl—INDICA TORS [SEC.1310<br />

cuits are properly matched, and the signal grids can therefore be in full<br />

operation at all times. Since it is essential that the proper d-c levels be<br />

maintained when the signal duty interval is large, d-c restorers must<br />

follow any a-c coupling. This circuit is often used as a single-channel<br />

switch, the signals being applied to one tube, and the other serving merely<br />

to cancel the plateau. The circuit may also be adapted to suppressor<br />

grid switching.<br />

13.10. Sawtooth Generators.—The sawtooth waveforms used as a<br />

basis for range sweeps and in certain varieties of precision timing circuits<br />

are practically always generated by a wave-forming network that is<br />

switched on and off by some sort of clamp.<br />

The basic action of all such devices can be illustrated by the simple<br />

circuit of Fig. 13.29. When S, a single clamp of proper polarity, is closed,<br />

an equilibrium state is reached in which X differs from ground potential<br />

E<br />

(1) Clym;;,g >T -+1 r<br />

+oli +on.<br />

R<br />

!<br />

~---- ----—- ==--—-.-<br />

x<br />

(2) Vx when<br />

l----m<br />

s<br />

(J<br />

.<br />

Rg<br />

c<br />

RC=T<br />

(3) V&:<br />

ifi::--<br />

Gnd<br />

-- —_____________<br />

T ----<br />

E<br />

FIG. 13.29.—Basicsawtooth generator.<br />

only by the small drop across R~. If S is suddenly opened, the current<br />

is “shifted from S to C, and the latter starts to charge exponentially at a<br />

rate determined by R, C, and E. The rising wave of the sawtooth is an<br />

exponential of time constant RC, as indicated in Waveform 2 of Fig.<br />

1329. If the sawtooth has an amplitude small compared to E—that is,<br />

if RC >> T—the rise is approximately linear (Waveform 3). Such sawtooth<br />

generators are widely used in cases where no great precision is<br />

required.<br />

When various sweep speeds are to be used, it is necessary to change<br />

the rate of rise of the sawtooth. This can be done in discrete fashion by<br />

switching the condenser, the resistance, or, within limits, the charging<br />

voltage. Continuous variation is most satisfactorily accomplished by<br />

using a rheostat for R (unless the control is remote) or by varying E<br />

through a potentiometer.<br />

Figure 13.30 illustrates both positive and negative sawtooth generators<br />

using single-triode clamps. If waves of both polarities are desired,<br />

the two circuits of this figure can be combined, or a single tube can be

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