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 conventional.
Straightforward designSince
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 circuitsAs 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 –4.8V 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 R48.
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. 3. Component layout of the printed-circuit board for the 300 W power amplifier.
Fig. 4. Track layout of the printed-circuit board for the 300 W power amplifier.
ConstructionBuilding
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.
FinallyHow
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 cable.
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.