PA300 power amplifier (Elektor 11/1995)

Design by A. Riedl

Taken by themselves, the properties of the PA300 amplifier are not revolutionary. But
taken in combination, they show something special: a robust 300 watt hi-fi power
amplifier that is not too difficult to build.

There are several starting points to the design of a power amplifier: pure hi-fi without any
compromise; simplicity and reliability; high output power. The design of the present
amplifier is a mixture of these. The result is a unit that does not use esoteric
components, is not too complex, and is fairly easily reproduced. In fact, it could well be
named a 'Hi-fi public address amplifier'.
There will be a few eyebrows raised at the power output of 300 watts (into 4Ohm); it
is true, of course, that in the average living room 30–40 W per channel is more than
sufficient. However, peaks in the reproduced music may have a power of 10–20 times
the average level. This means that some reserve power is desirable. Also, there are
loudspeakers around with such a low efficiency that a lot more than 30–40W is needed.
And, last but not least, there are many people who want an amplifier for rooms much
larger than the average living room, such as an amateur music hall.

Fig. 1. With the exception of an IC at the input, the circuit of the PA300 amplifier is

Straightforward design
Since every amplifier contains a certain number of standard components, the circuit of
Fig.1 will look pretty familiar to most audio enthusiasts. Two aspects may hit the eye: the
higher than usual supply voltage and the presence of a couple of ics. The first is to be
expected in view of the power output. One of the ics is not in the signal path and this
immediately points to it being part of a protection circuit. What is unconventional is an IC
in the input stage. Normally, this stage consists of a differential amplifier followed by a
voltage amplifier of sorts, often also a differential amplifier, to drive the predriver stages.
In the PA300, the entire input stage is contained in one ic, a Type NE5534 (IC1).
The internal circuit of IC1 is shown in the box on further on in this article. It may
also be of interest to note that the NE5534 is found in nine out of every ten cd players
(as amplifier in the analogue section). This is reflected in its price which is low. Its only
drawback is that its supply voltage is far below that of the remainder of the amplifier.
This means an additional symmetrical supply of ±15 V. Moreover, it restricts the drive
capability of the input stage. The supply requirement is easily met with the aid of a
couple of zener diodes and resistors. The drive restriction means that the amplifier must
provide a measure of voltage amplification after the input stage.

Circuit description
The input contains a high-pass filter, C5-R3 and a low-pass filter, R2-C6. The
combination of these filters limits the bandwidth of the input stage to a realistic value: it
is not necessary for signals well outside the audio range to be amplified – in fact, this
may well give rise to difficulties.
Opamp IC1 is arranged as a differential amplifier; its non-inverting (+) input
functions as the meeting point for the overall feedback. The feedback voltage, taken
from junction D7-D8, is applied to junction R4-R5 via R9. Any necessary compensation
is provided by C9, C12 and C14. The voltage amplification is determined by the ratio
R9:R5, which in the present circuit is x40.
The output of IC1 is applied to drive stages T1 and T3 via R6. These transistors
operate in Class A: the current drawn by them is set to 10 mA by voltage divider R10-
R13 and their respective emitter resistors. Their voltage and current amplification is
appreciable, which is as required for the link between the input and output stages.
The output amplifier proper consists of drive stages T6 and T7 and power
transistors T8, T9, T14, T15. which have been arranged as symmetrical power
darlingtons. Because of the high power, the output transistors are connected in parallel.
The types used can handle a collector current of 20 A and have a maximum dissipation
of 250 W.
The output stages operate in Class AB to ensure a smooth transition between
the n-p-n and p-n-p transistors, which prevents cross-over distortion. This requires a
small current through the power transistors, even in the absence of an input signal. This
current is provided by 'zener' transistor T2, which puts a small voltage on the bases of T6
and T7 so that these transistors just conduct in quiescent operation. The level of the
quiescent current is set accurately with P1.
To ensure maximum thermal stability, transistors T1–T3 and T6–T7 are mounted
on and the same heat sink. This keeps the quiescent current within certain limits. With
high drive signals, this current can reach a high level, but when the input signal level
drops, the current will diminish only slowly until it has reached its nominal value.
Diodes D7, D8 protect the output stages against possible counter voltages
generated by the complex load. Resistor R30 and capacitor C17 form a Boucherot
network to enhance the stability at high frequencies. Inductor L1 prevents any problems
with capacitive loads (electrostatic loudspeakers). Resistor R29 ensures that the transfer
of rectangular signals are not adversely affected by the inductor.

Protection circuits
As any reliable amplifier, the PA300 is provided with adequate protection measures.
These start with fuses F1 and F2, which guard against high currents in case of overload
or short-circuits. Since even fast fuses are often not fast enough to prevent the power
transistors giving up the ghost in such circumstances, an electronic short-circuit
protection circuit, based on T4 and T5, has been provided. When, owing to an overload
or short-circuit, very high currents begin to flow through resistors R25 and R27, the
potential drop across these resistors will exceed the base-emitter threshold voltage of T4
and T5. These transistors then conduct and short-circuit or reduce drive signal at their
bases. The output current then drops to zero.
If a direct voltage appears at the output terminals, or the temperature of the heat
sink rises unduly, relay Re1 removes the load from the output. The loudspeakers are
also disconnected by the relay when the mains is switched on (power-on delay) to
prevent annoying clicks and plops.
The circuits that make all this possible consist of dual comparator IC2,
transistors T10–T13, and indicator diodes D13 and D14. They are powered by the 15 V
line provided by zener diode D10 and resistor R42.
The 'ac' terminal on the PCB is linked to one of the secondary outputs on the
mains transformer. As soon as the mains is switched on, an alternating voltage appears
at that terminal, which is rectified by D12 and applied as a negative potential to T12 via
R50. The transistor will then be cut off, so that C20 is charged via R36 and R44. As long
as charging takes place, the inverting (+) input of comparator IC2b is low w.r.t. the non-
inverting (–) input. The output of IC2b is also low, so that T13 is cut off and the relay is
not energized. This state is indicated by the lighting of D13. When C20 has been
charged fully, the comparator changes state, the relay is energized (whereupon D13
goes out) and the loudspeakers are connected to the output. When the mains is
switched off, the relay is deenergized instantly, whereupon the loudspeakers are
disconnected so that any switch-off noise is not audible.
The direct-voltage protection operates as follows. The output voltage is applied
to T10 and T11 via potential divider R32-R34. Alternating voltages are short-circuited to
ground by C18. However, direct voltages greater than +1.7 V or more negative than –4.8
V switch on T10 or T11 immediately. This causes the +ve input of IC2a to be pulled
down, whereupon this comparator changes state, T13 is cut off, and the relay is
deenergized. This state is again indicated by the lighting of D13.
Strictly speaking, temperature protection is not necessary, but it offers that little
bit extra security. The temperature sensor is R39, a ptc (positive temperature coefficient)
type, which is located on the board in a position where it rests against the rectangular
bracket. Owing to a rising temperature, the value of R39 increases until the potential at
the –ve input of IC2a rises above the level at the +ve input set by divider R45-R46,
whereupon the output of IC2a goes low. This causes IC2b to change state, whereupon
T13 is cut off and the relay is deenergized. This time, the situation is indicated by the
lighting of D14. The circuit has been designed to operate when the temperature of the
heat sink rises above 70 °C. Any relay clatter may be obviated by reducing the value of
The terminal marked 'CLIP' on the PCB is connected to the output of IC1 via R31. It
serves to obtain an external overdrive indication, which may be a simple combination of
a comparator and LED. Normally, this terminal is left open.

Power supply
As with most power amplifiers, the ±60 V power supply need not be regulated. Owing to
the relatively high power output, the supply needs a fairly large mains transformer and
corresponding smoothing capacitors—see Fig. 2. Note that the supply shown is for a
mono amplifier; a stereo outfit needs two supplies.

Fig. 2. The power supply is straightforward, but can handle a large current. Voltage 'ac'
serves as drive for the power-on delay circuit.

The transformer is a 625 VA type, and the smoothing capacitors are 10 000 µF,
100 V electrolytic types. The bridge rectifier needs to be mounted on a suitable heat sink
or be mounted directly on the bottom cover of the metal enclosure.. The transformer
needs two secondary windings, providing 42.5 V each. The prototype used a toroidal
transformer with 2x40 V secondaries. The secondary winding of this type of transformer
is easily extended: in the prototype 4 turns were added and this gave secondaries of
2x42.5 V.
The box 'Mains power-on delay' provides a gradual build-up of the mains
voltage, which in a high-power amplifier is highly advisable. A suitable design was
published in 305 Circuits (page 115).
The relay and associated drive circuit is intended to be connected to terminal
'ac' on the board, where it serves to power the power-on circuit. If a slight degradation of
the amplifier performance is acceptable, this relay and circuit may be omitted and the
PCB terminal connected directly to one of the transformer secondaries.

Fig. 4a. Component layout of the printed-circuit board
for the 300 W power amplifier.

Fig. 4b. Track layout of the printed-circuit board
for the 300 W power amplifier.

Fig. 3. This close-up photograph shows clearly how the transistors
are fitted to the heat sink via a rectangular bracket.

Building the amplifier is surprisingly simple. The printed-circuit board in Fig. 4 is well laid
out and provides ample room. Populating the board is as usual best started with the
passive components, then the electrolytic capacitors, fuses and relay. There are no
'difficult' parts.
Circuits IC1 and IC2 are best mounted in appropriate sockets.
Diodes D13 and D14 will, of course, have to be fitted on the front panel of the
enclosure and are connected to the board by lengths of flexible circuit wire.
Inductor L1 is a DIY component; i consists of 15 turns of 1 mm. dia. enamelled
copper wire around R29 (not too tight!).
Since most of the transistors are to be mounted on and the same heat sink, they
are all located at one side of the board. However, they should first be fitted on a
rectangular bracket, which is secured to the heat sink and the board—see Fig. 3. Note
that the heat sink shown in this photograph proved too small when 4 Ohm loudspeakers
were used. With 8 Ohm speakers, it was just about all right, but with full drive over
sustained periods, the temperature protection circuits were actuated. If such situations
are likely to be encountered, forced cooling must be used.
As already stated, temperature sensor R39 should rest (with its flat surface)
against the rectangular bracket. On the board, terminals 'A' and 'B' terminals to the left of
R39 must be connected to 'A' and 'B' above IC2 with a twisted pair of lengths of
insulated circuit wire as shown in Fig. 3.
The points where to connect the loudspeaker leads and power lines are clearly
marked on the board. Use the special flat AMP connectors for this purpose: these have
large-surface contacts that can handle large currents. The loudspeaker cable should
have a cross-sectional area of not less than 2.5 mm2.

How the amplifier and power supply are assembled is largely a question of individual
taste and requirement. The two may be combined into a mono amplifier, or two each
may be built into a stereo amplifier unit. Our preference is for mono amplifiers, since
these run the least risk of earth loops and the difficulties associated with those. It is
advisable to make the '0' of the supply the centre of the earth connections of the
electrolytic capacitors and the centre tap of the transformer.
The single earthing point on the supply and the board must be connected to the
enclosure earth by a short, heavy-duty cable. This means that the input socket must be
an insulated type. This socket must be linked to the input on the board via screened
To test the amplifier, turn P1 fully anticlockwise and switch on the mains. After
the output relay has been energized, set the quiescent current. This is done by
connecting a multimeter (direct mV range) across one of resistors R25–R28 and
adjusting P1 until the meter reads 27 mV (which corresponds to a current of 100 mA
through each of the four power transistors). Leave the amplifier on for an hour or so and
then check the voltage again: adjust P1 as required.