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Electronics-World-1959-05

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ligible. Consequently, the voltage<br />

waveform at the output of the modulator<br />

and on the screen of the 807<br />

consists of positive half -cycles of audio.<br />

This is an important requirement. See<br />

"Transmitter Adjustments."<br />

Tests have shown that the power<br />

output of the 807 buffer on modulation<br />

peaks is four times that of the stage<br />

under conditions of no modulation or<br />

"idling." Also, with proper adjustment<br />

of R, as well as buffer and final amplifier<br />

grid drive (which is quite easily<br />

obtained), the resultant carrier power<br />

is proportional to the voltage change<br />

on the screen of the 807. (Note: This<br />

does not mean that the plate current of<br />

the 807 is also proportional to screen<br />

voltage change.)<br />

Resistor R, provides excellent load for<br />

the output circuit of the modulator. Its<br />

value is fixed at 25,000 ohms and requires<br />

no initial or periodic adjustment.<br />

Also, it will be noted that the resistor<br />

handles a maximum current of only 10<br />

to 13 ma., so that the power rating<br />

need be only 4 watts, and a minimum of<br />

source voltage is required.<br />

Design of R.F. Stages<br />

Conventional input and output circuitry<br />

is employed in buffer and final<br />

amplifier stages, as shown in Fig. 3. Important<br />

design requirements are: (a)<br />

sufficient drive for each stage to provide<br />

recommended operating grid current<br />

values for the type tubes used;<br />

(b) a fixed source of grid bias and<br />

screen supply voltage for the buffer<br />

and final amplifier; (c) complete isolation<br />

of stages to prevent both regenerative<br />

and degenerative feedback; and<br />

(d) provision for r.f. drive adjustment<br />

to both stages. Of course, the plate<br />

supply sources for both stages should<br />

have reasonably good regulation to<br />

prevent peak clipping. Also, the antenna<br />

system to be used with the<br />

transmitter should be capable of loading<br />

the transmitter to at least 75% full<br />

power output. Inadequate antenna<br />

loading results in a lower depth of<br />

modulation than is otherwise obtainable.<br />

The r.f. drive adjustment for the<br />

buffer, and to some extent for the final<br />

amplifier, is provided by the adjustable<br />

grid resistor R. Other methods can be<br />

employed for the purpose, of course,<br />

but if more than ample drive power is<br />

available from the preceding stage, the<br />

adjustable resistor method is particularly<br />

effective; moreover, it has the advantage<br />

of maintaining high efficiency<br />

in the buffer and thus high peak -power<br />

output from the stage. Optimum grid<br />

current values for the final amplifier<br />

can be obtained conveniently by readjustment<br />

of the tuned grid circuit.<br />

In fact, use of the tuned circuit in this<br />

manner is the preferred method of adjusting<br />

the grid current for the final<br />

stage.<br />

One more point should be mentioned<br />

in regard to r.f. design and that is the<br />

advisability of using a slightly higher<br />

"Q" in the plate circuit of the buffer<br />

and in the grid circuit of the final. This<br />

provides better load regulation for the<br />

N<br />

150<br />

LEGEND<br />

R.F DRIVE VARIATIONS<br />

UPWARD AT AUDIO FRED.<br />

I 1<br />

Fig. 4. How r.f. drive to power amplifier pre.<br />

vents p.a. cut -off, and constantly changes<br />

grid operating point at a.f. frequency.<br />

's<br />

r izo<br />

Slo<br />

Ñ T<br />

S<br />

U .<br />

,el 11<br />

5 45 50 55 60<br />

ANTENNA CURRENT<br />

65<br />

CLASS A82<br />

«.GLAS$ ADI<br />

I<br />

FOR<br />

Fig. 5. Actual antenna current values for<br />

several values of buffer screen voltage.<br />

large variations in r.f. current in these<br />

circuits.<br />

Final Amplifier Efficiency<br />

Fig. 6 is a diagram showing the pertinent<br />

elements and values of a 1 kw.<br />

input p.e.p. (peak- envelope -power)<br />

transmitter which is currently being<br />

used by the author on the 80 -, 40- and<br />

20 -meter phone bands. It was originally<br />

a 500 -watt rig, designed and built by<br />

the author in 1950, and utilized a pair<br />

of 803's in the final. QSO reports on the<br />

transmitter were excellent. In 1951 the<br />

803 tubes were replaced by the new<br />

and more efficient 4 -125A type tubes,<br />

Fig. 6. Shown at the<br />

right is the schematic<br />

diagram of the modulator,<br />

buffer, and the<br />

final power amplifier<br />

stage of the one -kilowatt<br />

(peak- envelopepower<br />

input) transmitter<br />

that is employed<br />

by the author. Refer<br />

to the text for a<br />

complete description.<br />

AUDIO FROM<br />

$PEECN AMP<br />

445 V)<br />

807<br />

R F DRIVER<br />

which were operated from the original<br />

clamp tube exciter at the 500 -watt<br />

p.e.p. input. Recently, however, the<br />

author obtained a new plate supply<br />

which provides the power increase.<br />

Since modulation is applied to the<br />

driver stage, it might be assumed that<br />

the final amplifier is necessarily operated<br />

as a class B linear. This, however.<br />

is not the case. Those who are<br />

familiar with the 4 -125A tubes will<br />

note that the grid bias value used is<br />

that specified by the manufacturer for<br />

class C c.w. operation. Also, the transmitter<br />

is initially tuned up for class C<br />

operation in the same manner as for<br />

any c.w. transmitter. This is possible<br />

because the system described is a form<br />

of "efficiency modulation," that is, the<br />

grid operating point of the final amplifier<br />

is constantly changing as modulation<br />

is applied to the preceding driver<br />

and remains at a fixed point only when<br />

no modulation is applied. Another very<br />

important reason is that modulation is<br />

applied to the driver, only in the form<br />

of positive cycles of audio, as explained<br />

under modulator operation. Thus, the<br />

driver screen (and plate) voltages<br />

never go negative with respect to the<br />

fixed d.c. potential ( "B + ") on the stage.<br />

This of course results in a grid operating<br />

point for the final amplifier which,<br />

although constantly changing, is never<br />

so far down on the plate current curve<br />

as to cause cut -off. Observation of the<br />

r.f. modulated waveform on an oscilloscope<br />

shows the negative modulation<br />

peaks to be only a small percentage of<br />

the amplitude of the positive peaks.<br />

See Figs. 4 and 5.<br />

While it is practical to adjust this<br />

system so that the carrier will be near<br />

zero with no modulation, it is not considered<br />

desirable. It can be seen that<br />

the average carrier power will be lower.<br />

Experience with this system of modulation<br />

has indicated that it is preferable<br />

to maintain an unmodulated carrier<br />

(Continued on page 144)<br />

4- 125A'S<br />

FA<br />

375 V (TOTAL CJRRENT 15 MA)<br />

ANT<br />

May. <strong>1959</strong> 61

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