Power amplifier 60W Class A
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There
is one amplifier configuration that is universally accepted as the ideal for audio use:
Class A operation . Many early amplifiers operated in Class A, but as output powers rose
above 10W the problems of heat dissipation and power supply design caused most
manufacturers to turn to the simpler, more efficient Class B arrangements and to put up
with the resulting drop in perceived output quality. Why Class A ? Because , when
biased to class A, the transistors are always turned on, always ready to respond
instantaneously to an input signal. Class B and Class AB output stages require a
microsecond or more to turn on. The Class A operation permits cleaner operation under the
high-current slewing conditions that occur when transient audio signal are fed difficult
loads. His amplifier is basically simple, as can be seen from the block diagram [Fig.1]. |
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The
simplified circuit [Fig.2] shows that each sub-amplifier
consists of two voltage gain stages. The first stage consists of a complementary
two�stage common emitter [Q1-7] whose gain is about x2.3. The second stage is a current
mirror stage [Q13-14] which drives the voltage across a load resistor tied to 0V. the gain
of this stage is about x200. Thus the overall open loop voltage gain is of the order of
x460 and so, as the closed loop gain is x26.7, the reduction due to negative feedback is
x17.2 or about 24db. The input amplifiers are powered from �
15V supply rails derived from R14-D1 and R21-D2. The current through the first stage [Q1]
is held constant, at about 0.36mA by the floating regulator stage [Q2-3] which provides
temperature compensation . The gain of this stage is set by emitter resistor R6 which
provides some local negative feedback. The second stage [Q4] is loaded by two series
cascode transistor [Q5-6], the first having its base tied to ground and the second having
its base tied to the �15V rail. Thus the maximum collector- voltage swing on Q4 is
greatly reduced , so reducing the effect of the base-collector capacitance [Miller effect]
which would reduce this stages high frequency bandwidth. In summary , the presence of Q5
and Q6 improves the bandwidth and linearity. The load on Q6 is one half [Q12] of the
current mirror and can be visualized as a resistor in series with a forward �biased
diode. The second half of the current mirror is a common-emitter stage [Q16-17], a simple
voltage amplifier except that its collector current equals [or ��mirrors��] the
collector current of the other half [Q12].This stage is made up of two transistor in
parallel which share the current. This arrangement was found to improve the linearity of
the stage. The other sub-amplifier [Q7 to Q14] works in exactly the same way but with
opposite polarity. The output stage uses the conventional Darlington emitter follower
arrangement, but with three parallel pairs of driver and output transistors. A transistor
Q15 is wired across the bases of the pre-driver transistors [Q18-19], providing a bias
voltage to set the standing current in the output stage. Q15 is mounted on the heatsink
with the aim of keeping this current constant regardless of temperature. The TR2 trimmer is used to set the value of this current.
The output DC offset voltage is set to zero by TR1 trimmer, in the input stage. In theory there should be no DC
offset at the output but, because of component tolerances and consequent mismatching ,
there always is. TR1 is arranged to make the current in the first stage of one
��sub-amplifier�� either higher or lower than in other and so null out any
residual offset. A simple low-pass filter is created by an RC networks at the input R2,C2
to reduce the bandwidth of the signal below that of the open loop amplifier and thereby
eliminate the generation of any transient intermodulation distortion.
The output stage is
quite substantial, using a total of six 250W power transistors. Fairly 'old- fashioned'
power transistors have been used [MJ4502/802 family] in preference to some of the higher
performance devices now available. They have been chosen because the die used to mount the
semiconductor junction is of a large area ; the device is quite rugged and can handle high
currents. The short term current capability of the output stage is, in fact, of the order
of 90A, somewhat in excess of the current capability of the wiring. The rest of
construction is equally massive with a steel chassis supporting six very large heatsinks.
However , construction is straightforward provided that the builder has strong arm muscles
and circuit alignment simple- there are but two adjustments- quiescent current and DC
offset voltage nulling.The coil L1 is wound onto the
body of R41. This is not a critical procedure- about 17 to 20 turnoff enameled copper wire
should do nicely. Particular care should be taken in mounting the power transistors. Good
quality insulating washers and bushes should be used and a generous smearing of thermal
paste is essential. These transistors should be bolted to the heatsinks very tightly to
ensure good thermal contact at all temperatures. One final point regarding construction.
Once the amplifier has been completed and tested, it should be switched on and allowed to
reach its normal operating temperature [about 20 minutes]. The amplifier should then be
switched off and all the screws tightened up. Differences in thermal coefficients of
expansion can result in some of the screws becoming slightly loose, particularly those
holding the heatsinks to the top and bottom covers.
My own proposal,
for whoever it decides makes the amplifier, is him it manufactures in two separate boxes,
one for each channel, [monoblock manufacture ], separating thus and the power
supply's. This will facilitate too much the mechanic and electrical manufacture. For
all the manufacture, is required certain relative experience, in these sectors. The sound
result is sure that it will vindicate, that tries, one and proportional performance
amplifiers in the trade, costs exceptionally expensively. ETI 8/81
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R1=47Kohm
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R31-32-35-36-39-40=0.22ohm
5W |
D1-2=15V
1.3W zener |
R2-9-27-28=1Kohm |
R41=10ohm
3W |
Q1-3-8-9-10-15-18=MPSA06 |
R3-18=10Kohm |
R42=10ohm
1W |
Q2-4-5-6-7-19=MPSA56 |
R4=18Kohm |
R43=5.6Kohm |
Q11-13-14=MPSA93 |
R5-13=3.9Kohm |
R44=330Kohm |
Q12-16-17=2N6515 |
R6-12=560ohm |
TR1=22Kohm
trimmer |
Q20-21-22=BD379 |
R7-8-19=2.7Kohm |
TR2=2.2Kohm
trimmer |
Q23-24-25=MJ802 |
R10-20=120ohm |
C1=10uF
16V |
Q26-27-28=MJ4502 |
R11=12Kohm |
C2=1.5nF
100V MKT |
Q29-30-31=BD380 |
R14-21=680ohm
0.5W |
C3-9-10=100pF
ceramic or Mylar |
L1=
see text |
R15-22-29-30-33-34-37-38=100ohm |
C4-5-6-7-8=100uF
25V |
F1-2=5A
fuse fast |
R16-17-23-24=220ohm |
C11-13=220uF
63V |
. |
R25-26=22Kohm |
C12=220nF
250V MKT |
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Power Supply for P.A 60w Class A |
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Power Supply Output Voltages |
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V1=� 40V |
V2=� 12V |
V3=� 50V |
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Here is the circuit of
power supply, for Power amplifier 60W Class A. He is one relatively simple and classic
power supply. In the line of input, exist, the classic circuit of protection and soft
start. In the circuit appear two transformers. This can change and all the coils they
become on one transformer. What it should we are careful, they are the cables that
transport power voltage � V1 [ �
40V ], are also big cross-section with investment of silicone, so that, they bear in the
currents that they will go through from in their, but also the temperatures in which they
will be found. The connections in the various points should become with screws. For other
two coils of transformer, does not need something particular. If you did not need the coil
of � 15V, we can suppress, also the supply of circuit of
protection, it become from the other coil of transformer. Attention should be given in the
region, round relay RL1, in primary of the transformer, which should also header well. The
bridge of rectifier BR1, should bolt in some point of chassis, so that is frozen. Obvious
is that will be supposed exist a transformer, for each power amplifier.
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Part
List For Power Supply |
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C1....4=15000uF
63V |
C15=33nF
630V |
S1= 2X2
switch 250V/10A |
C5-8=2200uF
25V |
BR1=Bridge
250V 35A |
IC1=7812
IC2=7912 |
C6-9=100nF
100V |
BR2=Bridge
250V 3A |
T1=230VAC//
2X28V AC - 500VA
//2X15V AC - 20VA
T2=230VAC // 2X35V AC - 40VA |
C7-10=47uF
25V |
BR3=Bridge
250V 3A |
C11....14=1000uF
63V |
F1=Fuse
3.15A slow block |
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Sam
Electronic Circuits 12/01 |
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