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Radar System Engineering

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SEC. 13.6] AMPLIFIERS 495<br />

by using a smaller value of Rk, which sacrifices gain, or by using a<br />

positive grid bias. The latter is usually to be preferred.<br />

3. To match the impedance of a cable. In this use the cable sees R,<br />

in parallel with the internal impedance of the circuit proper.<br />

Correct methods of matching are shown in Fig. 131 lc.<br />

Another special case of Fig. 13”1la is one in which the plate and<br />

cathode resistors are made equal, thus providing equal signals of both<br />

polarities from a unipolar input signal. Since the feedback ratio is unity<br />

for each output signal, this “split load” or” phase-splitting” amplifier has<br />

many of the desirable properties of the cathode follower, but the singlesided<br />

gain is always less and the internal impedance is greater.<br />

Amplifiers for Dejection-coil Currents.—Special problems are involved<br />

in producing rapidly changing deflection currents such as those involved<br />

in range sweeps, since the voltage across the coil may become very large.<br />

For a linearly increasing current (as in a range sweep) this voltage is<br />

given by<br />

di<br />

di<br />

‘z+ Ri=La+ Rat’<br />

where a is a constant. Since di/dt is also a constant the waveform consists<br />

of a step plus a linear increase. The sweep is usually produced by<br />

an increasing current since, except in special cases, this results in the<br />

minimum average current. As a result, the coil voltage drop during<br />

the sweep results in a decrease in the plate potential of the driver tube.<br />

The drop across the coil reaches its greatest value at the end of the fastest<br />

sweep, and the power-supply potential must be designed to accommodate<br />

this case. Such a sweep need not dissipate much power since the average<br />

current is low, but unfortunately the same power supply is used on high–<br />

duty–ratio sweeps where the average current is high. The total power<br />

dissipation due to the sweep circuit can be minimized by using a large<br />

number of turns on the deflecting coil and a correspondingly high supply<br />

voltage, since this reduces the losses in the driver tube and in the power<br />

supply itself. Usually, however, other circuits derive their power from<br />

the same supply, and a high voltage results in unnecessary dissipation in<br />

them. In consequence, the system is often designed in such a way that<br />

the plate of the driver tube operates on the margin of insufficient voltage<br />

on fast sweeps. Even if this were not the case, the amplifier would<br />

tend to discriminate against the higher frequencies because of the higher<br />

impedance offered by the coils to these frequencies.<br />

As a result of these factors good range sweeps can be obtained only<br />

with the use of greater negative feedback than would be necessary<br />

merely to correct for nonlinearities in the tube in a normal application.

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