Inside the Power Amplifier, Part 1
July 1959 Popular Electronics
are still a lot of vintage vacuum tube-based power amplifiers in
service. While this article from the July 1959 edition of Popular
Electronics focuses on an audio power amplifier, the principles
apply at least into the lower RF frequencies used by amateur radio
hobbyists and even commercial broadcast equipment. Fundaments of
waveform analysis and amplifier operations are covered. Distortion
is a prime concern for maintaining linearity at all frequencies,
unless you are working with some of the more modern saturated mode
transmitters, but hey, this is the pre-cellular realm.
July 1959 Popular Electronics
Wax nostalgic about and learn from the history of early electronics. See articles
published October 1954 - April 1985. All copyrights are hereby acknowledged.
Inside the Power Amplifier
By Joseph Marshall
previous articles in this series we have discussed the functions
performed by a hi-fi preamplifier. But when the preamp's job is
done, what have we? Only a puny little signal that is rarely more
than two volts, and more commonly in the neighborhood of one volt,
and - most important of all - with no power behind it. If you feed
this voltage to a speaker system, nothing will happen - no sound,
no nothing. Clearly, we need another link in our hi-fi chain, a
The purpose of the power amplifier is to
take the weak signal from the preamp and amplify it until it is
powerful enough to drive a loudspeaker system to the loudness level
of a symphony orchestra. And it must do this without changing the
signal. The first part of this task is not too tough; it is the
second part that enables audio engineers to make a comfortable living.
Disappearing Watts. The sound
level of a symphony orchestra can be reproduced in the
average living room with a power of about 0.5 acoustic watt. Unfortunately,
however, loudspeakers are inefficient devices. It may take anywhere
from 5 to 50 watts of audio power to drive some speakers to 0.5
acoustic watt, and as much as 100 audio watts to drive other speakers
to the level liked by some audio fans. At one time, 10-watt amplifiers
were thought to be the "ultimate" in power, but with the introduction
of several speakers with unusually low efficiencies, amplifiers
of higher power have become quite popular.
Although the maximum output of an amplifier is usually rated at
a frequency of 400 or 1000 cps, a hi-fi amplifier may have to deal
with signals from 20 to 20,000 cps. Therefore, it should be able
to deliver full output over the entire audio range. But it is a
lot harder to deliver full output at 20 and 20,000 cps than it is
at 400 or 1000 cycles. To get a flat response over the full range
at 10 watts, we may need an amplifier rated at 15 or more watts.
Fig. 1. Frequency response curves of typical low-priced amplifier
show that response at high and low frequencies suffers at high
power output levels.
Fig. 2. Negative feedback reduces distortion. In (A) original
signal is undistorted, but after passing through amplifier,
it appears as (B), with a "pip" on top. Portion of output is
fed back to input of amplifier out of phase with original signal
(C), and resultant input signal is shown in (D). "Pre-distorting"
the input signal allows resultant output (E) to follow original
input signal accurately.
Typical feedback circuit; feedback path is from plate of second
tube to cathode of first tube.
Fig. 3. Curve A above shows response curve of amplifier with
no negative feedback. If feedback is used in an amplifier which
has an inadequate frequency response, amplifier may become unstable,
as indicated by Curve B.
Fig. 4. Dyna "Mark III" power amplifier features a pentode voltage
amplifier direct-coupled to a triode split-load inverter. Both
functions are handled by one tube, a 6AN8.
Fig. 5. Mullard circuit as employed in the Eico HF-60 uses a
pentode voltage amplifier direct-coupled to a cathode-coupled
Fig. 6, Grommes 250K utilizes a 12AU7 as cascode voltage amplifier
followed by a 12BH7 cathode-coupled phase inverter.
Fig. 7, Acro "Ultra-Linear"II" has a cathode-coupled inverter
direct-coupled to push-pull triodes. This feature results in
an "all push-pull" amplifier.
Figure 1 shows the response curves of a typical low-priced
amplifier at various power levels. Curve A is the response at a
level of 1 watt, Curve B at 10 watts; and Curve G at the rated output
of 15 watts. Note that the amplifier delivers 15 watts between about
60 and 10,000 cps, but it delivers less than 15 watts at 20 and
20,000 cps. Therefore, although this amplifier can be honestly rated
by the manufacturer as a 15-watt job (at 1000 cps) , it does not
function as a 15-watt amplifier at the extremes of the audio range.
Negative Feedback. Although the maximum
output of hi-fi amplifiers is usually rated at the point where the
distortion reaches 2%, it is generally agreed that amplifier distortion
should not exceed 0.5% at any point in the audio range. Negative
feedback is the major distortion-reduction tool of the audio designer.
The principle of negative feedback is shown in Fig. 2. In
Fig. 2 (A) we have the original signal, pure and undistorted; but
when it comes out of the amplifier as shown in Fig. 2(B), it has
a peak or "pip" on it.
Now suppose we take a portion of
the output signal and apply it to the input tube of the amplifier
in parallel with the input signal, but exactly out of phase with
it. See Fig. 2(C). Because the signal we feed back is in reverse
phase, it will subtract from the input signal and reduce its amplitude.
Clearly, it will reduce the amplitude more at the point where the
peak in the feedback signal appears, and, in fact, will put a dip
at the exact point where the amplifier puts a peak. The resultant
signal at the grid of the input tube is shown in Fig. 2(D). When
this signal goes through the amplifier, the peaking. effect of the
amplifier fills in the dip we have created, and the resulting output,
shown in Fig. 2(E), although of lower amplitude than that of Fig.
2(B) , is almost as pure as the input signal.
Thus, by "predistorting"
the signal at the input, feedback compensates for the distortion
of the amplifier. Although it's never possible to eliminate distortion
entirely, if we use enough feedback we can come very close to it.
For example, we can take an amplifier that delivers 15 watts with
2.5% distortion and, by adding 20 db of feedback, we can theoretically
reduce the distortion to 0.25%.
Negative feedback is not miraculous. Like anything else, it has
its limitations. The problem can be visualized by referring to Fig.
At Curve A we have the response of an amplifier without
feedback. Note the slopes at the two ends of the curve. One of the
hard facts of hi-fi life is that where there is a slope there is
also a phase shift. As we apply feedback to the ranges represented
by the two slopes, the phase of the feedback is no longer exactly
180° out of phase, but is either slightly greater or less than 180°.
If we go far enough, or if the slope is steep enough, we
come to a point where the feedback signal, rather than being out
of phase, is actually in phase. When in-phase signals are fed back,
we get a pair of peaks at the opposite ends of the audio spectrum,
as indicated in Curve B. When such peaks are present, the amplifier
is usually unstable and may be thrown into momentary or continuous
oscillation at the frequencies where the peaks occur. We can avoid
this by controlling the amount of feedback used in the circuit.
Obviously, the flatter the response of the amplifier before
feedback is applied, the more stable the amplifier will be when
we apply feedback. Therefore, the audio designer starts by designing
the best possible circuit without feedback. In fact, almost any
genuine hi-fi amplifier is fiat at least over the audio range even
without the feedback loop.
Now we undertake the problem
of keeping the amplifier's response fiat over a wide bandwidth.
At the low end, a sloping response is the result of time constants
in the circuit produced principally by the coupling capacitors between
stages. The fewer the coupling capacitors, the fewer the time constants,
and the less the slope. There are two ways to reduce the number
of coupling capacitors: (1) by reducing the number of stages that
have to be coupled; and (2) by direct coupling (no capacitors) between
stages. Almost all modern power amplifiers employ a combination
of these two methods.
Excluding the output stage, the power
amplifier usually has at least two stages: a phase inverter to convert
the single-ended audio signal to push-pull (to feed the push-pull
output stage); and a voltage amplifier stage. Most modern amplifiers
employ a voltage amplifier directly coupled to the inverter (or
vice versa) which is capacitor-coupled to the output stage. Thus,
we have only one time constant to affect low frequency performance.
Two major causes of a sloping high end response in the front
end of the power amplifier are: (1) the grid-to-plate capacitance
of the tubes which acts as a bypass around the tube at high frequencies;
and (2) capacitance from tube elements and wiring to ground. Obviously,
the fewer the stages, the fewer the bypass points; hence, reducing
the number of stages to a minimum helps the high end as well as
the bottom end.
Problems of tube capacitances are minimized
by using special miniature tubes designed for less capacitance than
larger tubes and by using pentodes rather than triodes. Pentodes
have very low capacitance and can provide response well above the
audio range. As a result, a high proportion of modern amplifiers
employ pentodes as voltage amplifiers.
Almost all commercial amplifiers today use either the split-load
or the cathode-coupled inverter.
In the split-load inverter,
the load is divided evenly between plate and cathode. The output
at the cathode is always 180° opposite in phase and equal to that
at the plate; therefore. we have the necessary push-pull signal
needed to drive a push-pull stage. This inverter is simple and inexpensive.
it has low distortion. and with carefully matched plate and cathode
resistors. it is capable of well-balanced output. The split-load
inverter, however, provides no signal gain.
In the cathode-coupled
inverter, a high-mu twin-triode is usually employed. The signal
is fed to one triode which operates as a regular amplifier with
a large cathode resistor. The other tube operates as a grounded-grid
amplifier, obtaining its input from the cathode of the first tube.
Outputs from the plates of the two triodes are 180° out of phase,
and thus, again, we have the needed push-pull signal to drive the
output stage. This inverter can be designed for considerable gain.
Typical Circuits. A very successful circuit
first used in the Dyna amplifiers is diagrammed in Fig. 4. Here
we have a pentode as the input tube/voltage amplifier direct-coupled
to a triode split-load inverter. Both the triode and the pentode
are part of a single 6AN8 tube. The bandwidth of this circuit is
very wide and has very small losses at both low and high frequencies.
Given a good output transformer, it is no trick to obtain 20 or
30 db feedback with it. This circuit supplies the 30-55 volts of
signal to drive the larger output tubes, such as the EL34, KT88,
lower powered amplifiers, a triode is sometimes substituted for
the pentode because the tubes (usually the EL84) used in these amplifiers
need fewer volts of drive. A twin-triode is generally used; one
half for the amplifier and the other half as the inverter.
Another popular circuit is the so-called "Mullard" configuration
shown in Fig. 5. Again we have a pentode voltage amplifier, direct-coupled
to a twin-triode cathode-coupled (or long-tailed pair) inverter
which is capacitor-coupled to the output stage. This circuit has
more gain that the Dyna circuit, but losses at very high frequencies
are slightly greater. Here, again, a triode is sometimes substituted
for the pentode in lower powered amplifiers.
circuits are used in probably 90% of the power amplifiers on the
market, but there are a number of interesting variations. In Fig.
6 we have a circuit used by Grommes which employs a twin-triode
as a cascade voltage amplifier. The cascade has most of the virtues
of the pentode and, in addition, is perhaps a little more stable.
The cascade voltage amplifier feeds a cathode-coupled inverter.
In Fig. 7, in a circuit used by Acro, we have a cathode-coupled
inverter at the input which is direct-coupled to a push-pull pair
of triode amplifiers. This results in an amplifier that is push-pull
from beginning to end. Feedback from a special winding on the output
transformer is applied to the inverter grid, which is normally at
Though each of these circuits has
its own advantages and disadvantages, all are capable of producing
superb performance. But overall design, not the design of any single
circuit, determines the end quality of an amplifier. Next month
we will consider the design of power output stages and the part
it plays in the over-all circuitry of an amplifier.