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Radar System Engineering

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SEC.12.6] VIDEO AMPLIFIERS 451<br />

amplifier must recover from large signals quickly, requiring that<br />

no control-grid current be drawn on strong signals.<br />

3. Some form of limiting must be provided. The noise voltage at<br />

the output of the detector will be approximately 2 or 3 volts peak.<br />

In order that the noise be clearly visible on the screen, it must be<br />

amplified sufficiently to drive the indicator tube over something<br />

like half its allowable control-grid voltage swing. Since signal<br />

voltages from the detector may be 20 volts or more, the output<br />

voltage must be limited so that the indicator will not be driven<br />

outside its allowable range of voltage.<br />

The simplest and most commonly used type of video amplifier is the<br />

resistante-capacitance-coupled am-<br />

6+<br />

plifier shown in Fig. 12.10.<br />

64C7<br />

Although the gain for small sig-<br />

c, 6AG7<br />

nals can be simply exp~essed in terms + ‘= ~<br />

---<br />

:<br />

of the tube and circuit constants, it<br />

-L<br />

.~. To<br />

is usually determined by reference to<br />

R<br />

terminated<br />

.-_L_- ‘ R,<br />

the characteristic curves of the tube.<br />

CB - line<br />

For many reasons, the high-frequency<br />

8[*<br />

performance is most conveniently<br />

expressed by giving the frequency<br />

at which the gain is down 3 db (voltage<br />

down to 0.707). This will be<br />

referred to as the “ cutoff frequency. ”<br />

For the amplifier shown thi~ occurs when<br />

j=-!L<br />

23rRC’<br />

= =<br />

R=<br />

B+<br />

FIG. 12,10.—Video amplifier.<br />

where R = parallel resistance of R= and R~, and C is the total capacity to<br />

ground which includes output and input capacities plus stray capacities.<br />

Again the need for keeping the stray capacity to a minimum is apparent.<br />

This is sometimes difficult when large coupling condensers or lohg leads<br />

are involved.<br />

There are other coupling networks that will increase the cutoff frequency<br />

and yet preserve the same gain. Perhaps the simplest of these<br />

is the “shunt peaking” circuit, which uses an inductance in series with<br />

the load resistor, RP. Let the parameter M be defined by the equation<br />

L = il{R2C. (12]<br />

Then M can be used as a measure of the performance of the circuit.<br />

Since a value of M = 0.25 corresponds to critical damping, it produces<br />

qo overshoot and yet increases the cutoff frequency by a factor of 1.41.<br />

A value of M = 0.41 is the highest that can be used without puttinga hump<br />

(11)

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