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The Class-A Amplifier =
Site
This
page was last updated on 13 January 2002
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Modular Pre-Amplifier Design
(Wireless World, July =
1969)
Optimally designed =
stages that=20
may be used separately or in several different combinations
by J. L. Linsley =
Hood,=20
M.I.E.E.
The type of distortion introduced by a class A transistor amplifier =
operating=20
at a low signal level will be predominantly second harmonic and =
inoffensive to=20
the ear. Although harmonic distortion is a convenient thing to measure, =
and=20
makes a reasonable yardstick for comparative purposes, at low levels its =
presence is less important than that of the intermodulation effects it =
causes.=20
When a complex signal is transmitted through a non-linear element,
intermodulation products between the separate components of the signal =
are
formed, and these are readily apparent in the final audible result as a =
=93blurring=94, and the loss of separate identity, of the individual =
components=20
which make up the whole. A measure of this is the ease (or difficulty) =
in
distinguishing the words of a choral performance in the presence of an
orchestral background, or in identifying the presence and nature of =
individual
instruments in a large orchestra.
Measurements by a number of workers (1)
have indicated that the magnitude of intermodulation products can be =
much
greater than that of the total harmonic distortion level, and the
non-linearities which are likely to be of the most importance in this =
respect
are those at the low- and high-frequency ends of the audible range.
At the moment, the performance of audio amplifiers is much superior =
in this
respect to that of f.m. transmissions, tape recordings, disc replay =
systems, or
loudspeakers. However, advances in manufacturing techniques of =
gramophone
records, pickup cartridges and loudspeakers have allowed a continuing
improvement in the performance of these in harmonic and i.m. =
distortion, and it
is clear that any amplifier design offered at this time should have a =
very high
standard of performance if it is to remain of continuing value over the =
next
decade.
Fig. 1. A likely =
combination of=20
stages.
(Click on figure for a higher resolution=20
image)
The author has designed a range of high-quality pre-amplifier stages. =
Each
stage performs its required operation with negligible noise and =
distortion.
When joined together, as for example in Fig. 1, the total harmonic =
distortion
level is below 0.1% over the frequency range 20Hz-20kHz, at any tone =
control
setting, and for up to 2V r.m.s. output. Each stage is capable of =
operating on
its own and has an output impedance low enough for screened cable
inter-connections to be made without high frequency loss.
Magnetic pickup equalization circuit
Fig. 2. =
Phase-inverting amplifier=20
stage used to obtain R.I.A.A. replay characteristic.
The required R.I.A.A. replay characteristics can be approximated by =
several
different circuit arrangements. The most straight-forward from the =
point of
view of performance calculation is that shown in Fig. 2, employing a =
simple
phase-inverting amplifier stage. If the gain of amplifier M is high =
enough,
point Z becomes a virtual earth (see Appendix I), and the input =
impedance of
circuit equivalent to that of the input network B. The load resistance =
required
by the pickup cartridge, usually 47-50kohm, is provided by a suitable =
choice of
R1. With resistor R2 equal to R1, stage gain is given by R4 + R5/R5 at =
the
mid-point frequency (usually 1kHz) if the impedance of C2 is large, and =
that of
C3 small in relation to R2. Since the voltage output to be expected =
from most
good quality magnetic pickup cartridges is in the range 4-10mV for a =
5cm/sec
recorded velocity, a gain of 10 is adequate for this stage. The =
required replay
frequency-response curve shown in Fig. 3 can be obtained by a suitable =
choice
of C2 and C3. Since the two networks A and B determine the frequency =
response
of this circuit, it is apparent that substitution of these can be made =
to
provide a wide range of different performance characteristics without
alteration to the circuit of amplifier unit M.
Fig. 3. Required =
R.I.A.A.=20
frequency-response curve and circuits approximation to this.
The final circuit can be seen at the front of Fig. 1. Because phase =
inversion=20
between input and output is required, and because the necessary gain is =
higher=20
that can be obtained from any single transistor arrangement, a triplet =
circuit=20
has been used. Tr1 and Tr3 are high-gain, low-noise voltage-amplifying =
stages,=20
and Tr2 is a phase and voltage transformation stage allowing the input=20
transistor to be used in its most linear region. The output transistor =
has a low=20
collector load resistance, to reduce distortion to the lowest possible=20
level.
D.C. working-point stability is ensured by D.C. negative feedback =
through R3
and R2 to the base of Tr1, and through R4 to the emitter circuit of the =
same
transistor. The circuit R4, C4, and C5 also provides the feedback path
necessary, in conjunction with the input capacitor C1, to provide an
18dB/octave steep-cut rumble filter, with a turn-over frequency of 25Hz =
(see
Appendix II), and an ultimate attenuation of more than 40dB at 8Hz.
Capacitor C6 provides phase correction, and is essential for a clean
square-wave response, and freedom from transient ringing, when used =
with a
capacitive load.
The response of this circuit is particularly good, and it can deliver =
up to 1=20
volt output with distortion less than 0.02% from 100Hz to 10kHz.
Stages for ceramic cartridge equalization
Fig. 4. Impedance =
conversion stage=20
for use with ceramic cartridge. This may be
directly substituted for =
the=20
magnetic cartridge stage at the front of Fig. 1.
Fig. 4 is an impedance conversion stage contributing less than 0.05%
distortion at 1kHz and having a flat response from 35Hz to greater than =
200kHz,
with 18dB/octave roll-off below 35Hz. This simple stage may be directly
substituted for the magnetic cartridge stage of Fig.1.
Alternatively, should it be required that the pre-amplifier be able =
to cope
with inputs from both magnetic ceramic cartridges, then switchable =
equalization
networks for A and B can be provided. These are shown in Fig. 5. When =
used with
a ceramic cartridge the output is from 50 to 200mV. To preserve the =
required
shape of the rumble filter characteristic it is necessary to alter the =
values
of C4 and C5 from 25uF to 12.5uF. The pre-amp response is then as shown =
in Fig.
5, curve 1.
Fig. 5. Changes in =
equalization=20
networks A and B of the magnetic cartridge
input stage allowing =
direct use of=20
ceramic cartridge. Components for network
"A" are the same for the =
three=20
curves shown.
The performance of many ceramic pickup/amplifier combinations is
disappointing in comparison with that obtainable from a good magnetic =
cartridge
with a similar amplifier. This is sometimes due to the mismatching =
between
cartridge and amplifier, or through inadequate input impedance =
provision (in
the modification shown in Fig. 5 this is 4.4Mohm), or due to the =
failure of the
piezoelectric element within the cartridge to provide the required =
equalization
for the 12dB fall in voltage output anticipated when a recording having
R.I.A.A. velocity characteristics is replayed on a displacement =
sensitive
device. In the latter case, a very considerable improvement in the =
relative
performance of the ceramic cartridge may be obtained by shunting part =
of the
input resistor in the input network B by a small capacitor. Curves 2 =
and 3 in
Fig. 5 show partial and complete correction respectively.
Tone-control stage
The tone-control stage is of conventional type, and uses a negative =
feedback
system derived from the design due to Baxandall (2). However, it differs from normal =
practice in=20
that a junction field-effect transistor is used as the active element.=20
Field-effect transistors have both lower noise levels and better =
linearity than=20
bipolar transistors, and in this type of circuit the high input =
impedance=20
results in negligible loading of the tone-control network. The stage =
gain needed=20
in this circuit requires a high value drain load resistor, and the =
f.e.t. must=20
therefore be followed by an emitter-follower to provide the low output =
impedance=20
desired for easy interconnection of the separate units.
If the feedback tone-control network is to perform satisfactorily, =
both the
input and output impedances seen by the network at its ends must be low =
in
relation to the network input impedance when the sliders of the =
potentiometers
are at the position nearest to the point being measured. Some form of =
impedance
conversion circuit is therefore also needed between the volume control =
and the
tone-control circuit. An emitter follower is also used at this point. =
The
0.001uF capacitor in the emitter circuit of Tr4 is to avoid the =
possibility of
high frequency parasitic oscillation occurring if long screened leads =
are used
to connect the base of Tr4 to the volume control.
The input to this section is taken through a switch from the =
gramophone
pre-amplifier section, and other inputs provided with preset =
gain-equalization
potentiometers. The switch is arranged to earth the inputs not in use, =
to
minimize breakthrough between programme channels.
The gain/frequency characteristics of the stage are shown in Fig. =
6.
Fig. 6. Gain/frequency =
characteristics of tone control stage.
Low-pass filter circuit
The voltage amplifying stage preceding the main amplifier should =
include a
steep-cut low-pass filter that can be set to remove unwanted high =
frequencies.
This can be done either by a suitable LCR filter arrangement, or by an =
active
filter giving an equivalent performance without the use of inductors. =
The
circuit arrangements available for low-pass active filters are shown in =
Fig. 7.
(b) is the well known circuit arrangement first employed in an audio =
amplifier
design by P. J. Baxandall (3), =
and (d) is
the unity gain rearrangement of this circuit introduced by Sallen and =
Key (4). The frequency response of all =
these circuit
arrangements is similar, mutatis mutandis, to that shown in Fig. =
8, and
the circuit should be preceded or followed by a simple RC filter if the =
type of
response shown in the dotted line is required.
Fig. 7. Circuit =
arrangements for=20
active low-pass filter design.
Fig. 8. Frequency =
response of the=20
active filter circuits is 12dB/octave. Preceding
the filter with RC =
network gives=20
response shown in broken line.
For a given overall stage gain, type (b) gives much better distortion =
factor
near the region of cut-off than (a), and (c) is marginally better than =
(b) when
used with non-linear amplifier elements. The particular advantage of =
(c)
however, is that it can be used conveniently with a very low-distortion
two-transistor circuit.
The final stage, with the filter circuitry, is shown in Fig. 1. As a =
matter
of practical convenience, the component values of this circuit have =
been chosen
so that the required low-pass response is obtained when all of the =
capacitors=20
=92Cx=92 are of equal value to each other. The frequency response =
obtained with a
given value of =91Cx=92 can be found in Fig. 9. The user can =
interpolate between
these to obtain turn-over frequencies at any points to suit his own
requirements. If a ganged selector switch is employed to give a range =
of
turn-over frequencies, the switch arms (moving contacts) should be =
connected to
the junction of the resistors in the RC filter and to the 470ohm =
resistor in
the main filter network. In Fig. 1 the 0.0047uF capacitor for =91Cx=92 =
results in=20
response being 3dB down at 18kHz. With good quality programme sources =
this is a
recommended capacitor value.
Fig. 9. Graph and =
table of=20
turn-over frequencies for different value of =91Cx=92.
With capacitors of zero value, the response of the circuit is flat to =
about
100kHz. The user should however arrange for the response to fall off =
above
25kHz. (It is unlikely that the listener will find anything to gain =
from the
parts of the sonic spectrum beyond this point.)
The optimum performance of this particular type of circuit =
arrangement is
obtained when the overall gain is about 50 with feedback. A 20-40mV =
input is
therefore adequate for this stage for the output voltages required.
The distortion level of this circuit is less than 0.03% at 2 volts =
r.m.s.
output or less, at any frequency within the pass band. The output =
impedance is
less than 150 ohms over the range from 20Hz to the cut-off frequency=20
selected.
It is convenient, for several reasons, to operate at the 60-100mV =
level
through the tone-control stages. At this output voltage level the =
distortion
introduced by a RC coupled f.e.t. stage is less than 0.1% even without
feedback, so that the maximum =91lift=92 settings of either =91bass=92 =
or =91treble=92=20
controls cannot give rise to unacceptable levels of distortion. It is =
also large=20
enough for the noise and inevitable 50Hz pickup to be unobtrusive. Some
attenuation is therefore desirable between the tone control unit and =
the
steep-cut filter circuit. This is obtained by the preset 2kohm =
potentiometer in
the tone control circuit, which provides a convenient means for setting =
the
overall gain of the amplifier system, and also as a coarse =91balance =
control=92 in
a stereo system. Fine balance between channels is obtained by adjusting =
the
100ohm balance potentiometer in the output stage. This alters the stage =
gain
over the ratio 6:10.
Constructional notes
The constructional technique used by the author in building the =
prototype of
this amplifier is similar to that used in the 10-watt class-A design =
described
in Wireless World in April 1969, with the separate units laid out in =
mirror
image form, as a stereo pair on a single 4in X 4=BEin s.r.b.p. pin =
board, Two
units of each type can be accommodated on each board, laid out more or =
less in
the form of the circuit diagram(or its mirror image).
In general, reasonable care should be taken to separate input from =
output
leads, and where the boards are to be mounted as a group within the =
same box,
it would be wise to interpose a sheet metal screen between them.
The units are separately coupled by 250uF capacitors from a common =
24-volt
line, derived from a zener diode stabilized RC filter power supply. =
This supply
is separate from the main amplifier, and a 30mA output is ample. =
Details of a
suitable power supply are given in Fig. 10. The expected working =
voltage on
each of the unit sub-rails is about 15volts.
Fig. 10. Suitable =
power supply for=20
any combination of stages.
Apart from the input transistor in the gramophone pre-amp unit (Tr1) =
for
which the BC109 is to be preferred, there is no particular reason why =
any
modern silicon planar types should not give an indistinguishable =
performance.
For example, the n-p-n types could be 2N3904, BC107/8/9, 2N3707, or =
BC184Ls.
Similarly, the p-n-p types could be 2N4058, 2N3906, or BC214Ls.
Although, in many cases, the use of 1/4 watt resistors is sufficient, =
it
would probably be found simpler to use 1/2 watt units throughout. 5% =
tolerance
carbon film resistors are to be preferred.
The author has mounted the gramophone pickup equalization circuit in =
a
separate small diecast box, immediately under the gramophone turntable =
unit, so
that the leads from the gramophone are taken at a low impedance from =
the output
of this unit. This has been very effective in reducing the hum picked =
up on the
output leads to an imperceptible level.
Appendix l
The use of =91virtual earth=92 (null seeking) amplifier circuit =
arrangements is
superficially ill-advised with input elements such as pickup =
cartridges,
because it appears that as the operating frequency is increased, the =
input half
of the balancing limbs will also change, with a resultant change in the =
gain of
the circuit. In particular a magnetic pickup cartridge may have an =
inductance
of some 300-800mH and the impedance of this will exceed that of the =
input
circuit in the range 12-20kHz. This should clearly reduce the gain of =
the
system by reducing the ratio of A to B.
However, on reflection, it can be seen that the amplifier operates as =
a null
generating device, sensitive only to the current flowing in the input =
circuit
to the =91virtual earth=92. As the operating frequency increases, so =
the current
flow through R1 will decrease, but so it would in any case, regardless =
of the
amplifier, were the element simply connected across network B as the =
load
recommended by the cartridge manufacturers (at these frequencies the =
impedance
of C1 can be ignored), and the voltage across R1 measured by a perfect =
voltage
amplifier. The decrease in current input into a given resistive loads =
from a
source having a series inductance is simply an unfortunate fact of =
life, from
which one cannot escape, whatever one=92s technique of measurement, and =
high
impedance voltage amplifiers connected across the load, or low =
impedance
current amplifiers connected in series with it, are alike in this =
respect,
except that with transistors, the latter are a bit easier to contrive. =
The same
argument is also applicable, in the appropriate context, to high =
impedance
capacitative elements such as piezo-electric pickup cartridges. Once =
again, the
voltage amplifier and current amplifier see the same phenomena in =
identical
form. The necessary, and inevitable, corrections can be accomplished by =
simply
by the tone control settings.
Appendix II
Although the R.I.A.A. replay characteristics suggest an approximately =
flat
velocity response from 20-50Hz, this would effectively imply recording =
bass
lift in this region and the author suspects that this is not done and a
constant modulation characteristic being used instead. The author has
therefore, for his own use, modified the values of the feedback =
elements as
follows: R5 =96 470 ohms; R6 =96 1.5kohms; C1 =96 0.47uF; C3 =96 =
6800pF; and C6 =96=20
6800pF. These changes maintain the velocity response flat down to 25Hz, =
with
rapid attenuation below this frequency. Unfortunately the mid point =
gain of the
circuit is reduced to 5, and some additional amplification is therefore =
needed
if it is desired to avoid working with the tone control circuit at the =
20mV
level. The simple floating emitter collector-follower circuit of Fig. =
11 is
therefore interposed, without coupling capacitors, between the output =
series
resistor and the collector of Tr3. The distortion contributed by this =
is less
than 0.05%.
Fig. 11. Floating =
emitter=20
collector-follower circuit referred to in Appendix II.
References
1.
Langford-Smith, F., =93Radio Designers Handbook=94, Vol.4 =
ch.72.
2.
Baxandall, P. J., =93Negative-Feedback Tone Control=94, Wireless =
World,
October 1952
3.
Baxandall, P. J., =93Gramophone and Microphone Pre-amplifier=94, =
Wireless
World, January 1955
4.
Sallen, R.P. and Key, E.L., I.R.E. Trans. Circuit Theory, March =
1955, p.
74-85
Postscript (December =
1970)
Modular pre-amplifier
The intention in the original article was not to offer a complete
pre-amplifier design, but rather to describe a series of versatile =
=91building
blocks' from which the potential user could assemble a 'custom built=92 =
pre-amplifier to suit his own needs or preferences. To increase the =
scope of
this some additional circuit modules are described below.
Steep cut low-pass filter. It is certainly prudent to =
include a=20
low-pass filter somewhere fairly close to the input of the main =
amplifier
whenever a wide-bandwidth main amplifier is to be used with a =
good-quality=20
loudspeaker system. Doing so will prevent unwanted high-frequency =
components,=20
arising from component noise, record surface noise, and similar causes, =
from=20
impairing the long-term listening comfort of the user, and from =
producing=20
avoidable intermodulation effects due to non-linearities in the=20
loudspeakers.
The combination of such a steep-cut low-pass filter with a =
low-distortion,
low-output impedance driver stage, with a gain of 50 and an output =
capability
of some 2V r.m.s. at 0.02% t.h.d., appeared to provide the most =
versatile
system for use with a wide variety of power amplifiers.
However, many power amplifiers require an input voltage of only 0.25 =
- 0.8V
r.m.s., and there are snags in respect of hum and component noise if =
the stages
following the volume control are operated at levels below some 50mV. =
The
preferred level to achieve an optimum balance of noise and distortion
components is probably in the 100 =96 200mV region. In these =
circumstances a
driver-stage gain of 50 is excessive, and much of the available gain =
must be
removed by an input attenuator, and if a potentiometer is used for this =
it can
introduce noise.
To meet this need more conveniently, two further versions of the =
driver
amplifier, incorporating steep-cut low-pass filter characteristics =
which are
identical to that of the original circuit, and having gains of 20 and =
5, are
shown in Figs. 5(a) and 5(b). An alternative, three-transistor =
arrangement
whose cut-off slope is variable over the range =966 to =9618dB/octave, =
at any
chosen (switchable) frequency, is shown in Fig. 6. This consists of a =
single
transistor version of the =91H=92 filter used in the two previous =
pre-amplifier
designs (the nomenclature derives from the shape of the component =
layout in the=20
=91op-amp=92 form), followed by a very low distortion two-transistor =
amplifier whose=20
gain can be chosen as required, over the range 5 to 100, by adjustment =
of Ra and=20
Rb. If a unity-gain stage is all that is required (actually the gain is =
about=20
0.9) the output ran be taken from the point marked 'A' on the diagram, =
and Tr7=20
and Tr8 omitted.
The response curve of the filter circuit, at any chosen turnover =
frequency is=20
shown in Fig. 7. The slope is smoothly variable by adjustment to the =
5kohm pot.=20
If the slope pot. Is open circuit the response is flat to 20kHz and =
beyond, but=20
in this case the load impedance should not be less than 50kohm.
For completeness, an equivalent single-transistor high-pass filter, =
having a
cut-off slope approaching 18dB/octave, and suitable for use as a =
=91rumble=92=20
filter or a pre-amplifier woofer/tweeter cross-over filter, is shown in =
Fig. 8.
The frequency response characteristics of this filter are shown in Fig. =
9. Both
of these filter circuits should be driven from a source having a fairly =
low
impedance =96 not higher than 6kohm.
If single transistor =91H=92 filters are to be used at output signal =
levels
exceeding 100mV a Darlington transistor, e.g. Motorola MPSA14, is to be
preferred.
The apparent noise level, referred to the input, of the two =
transistor driver=20
amplifiers, using reasonably low noise transistors and an input =
impedance of the=20
order provided in the normal circuit, is about 4 =96 6uV. The output =
noise voltage=20
in the original circuit was 0.2 =96 0.3mV, which should be inoffensive. =
With a=20
lower gain driver stage this noise will be reduced even further.
The use of a variable negative feedback type of balance control in =
these
circuits is deliberate, in that it permits a low output impedance to be
obtained from the driver stage. Measurements made with a wide range of
published transistor-operated power amplifiers have shown that =
substantially
lower distortion levels are often given by using a low-impedance drive =
circuit,
and that there is frequently an advantage also in terms of hum, noise, =
and
transient response.
Tone-control circuit. This stage has a worst case (bass and =
treble
controls set to maximum =91lift=92) distortion level which is typically =
less than
0.1% at 1V r.m.s. output. It is perfectly capable of driving a normal=20
high-quality power amplifier without the interposition of other =
pre-amplifier=20
stages. The required signal amplification could then be provided prior =
to the=20
volume control. This is tending to be the normal practice in commercial =
=91hi-fi=92=20
amplifiers, in that it gives the highly-sought-after zero noise-level at =
minimum=20
volume control settings, and makes for economies in the use of =
components.
Noise in the tone-control stage due to the f.e.t. has caused =
occasional
troubles. This should not occur with the f.e.t. now recommended for =
this part
of the circuit (the Amelco 2N4302), which appears to have a =
consistently low
noise level. The necessary bias adjustments were described in a letter =
to the
editor published in April 1970.
The input impedance level suggested for the tone-control stage was =
50kohm,
because it was thought that most of the other systems likely to be used =
with
this unit would be transistor operated; and this would be a suitable =
level for
this purpose, while avoiding some of the hum pick-up problems likely to =
be
encountered at higher impedance levels. However, if this impedance is =
too low,
and if a high gain (beta greater than 400) transistor is selected for =
Tr4 =96 in
fact most BC109s will do =96 the base bias resistors can be increased =
to 1Mohm
and 560kohm (instead of 200kohm and 100kohm) enabling the volume =
control and
auxiliary control potentiometers to be increased to 25kohm.
If an even higher input impedance is required, the f.e.t. impedance
conversion shown in Fig. 4 in the original pre-amp article can be =
substituted
in its entirety for Tr4. To preserve the function of the rumble filter =
in this
circuit, with the 0.47uF capacitor desired to feed the tone-control =
network, a
4.7kohm resistor should be connected from the output side of this =
capacitor to
the earth line. A low noise f.e.t. is of course preferable.
If additional amplification is required on any signal source prior to =
the
tone-control stage (if this is working at the 100mV level) a simple
single-transistor feedback amplifier such as that shown in Fig. 10, can =
be used
with confidence, in that its performance is stable, its noise is low, =
it is
almost impossible to damage by an input overload, and its distortion is =
well
below 0.1% at output voltages up to 0.25V r.m.s., and with gains up to =
10.
Magnetic pickup equalisation circuit. Some requests have been =
received=20
for component values for the use of this circuit for tape-replay =
characteristic=20
equalization. The author remains of the opinion that this type of =
provision is=20
best left to the manufacturers of the tape recorder, in that the actual =
head=20
characteristics can influence the replay frequency/voltage =
characteristics.
However, a fairly close approximation to the replay curve =
theoretically
required for 7.5 i.p.s. is given if C2 and R2 in the original =
equalization
network A are altered to I00pF and 27kohm.
The noise level of this circuit is almost entirely determined by the=20
performance of Tr1 The BC184C and 2N5089 transistor types may be of =
interest in=20
this position.
The maximum output which can be obtained from this circuit at 0.02% =
t.h.d.,
is 2V r.m.s. If the normal input to the tone control circuit, or other
following stages, is l00mV, this gives a 26dB overload capability. The =
gain of
the equalization circuit can be increased by a factor of 3, (i.e. to 30 =
at
1kHz) without upsetting the rumble filter characteristics if R5 is =
reduced to
68ohm and C4 increased to I00uF.
Miscellaneous. An omission from the original article was the
suggestion that high value resistors (2 =96 5Mohm) should be connected =
across the
switch contacts, from slider to each Cx. This removes 'plops' on =
switching
ranges.
A number of correspondents have queried the need for a separate h.t. =
power
supply for the pre-amp. (The reservoir capacitors for the unit shown =
should
have read 35V working, not 25V). It is always possible to run the =
pre-amp via a
suitable voltage-dropper circuit from the main amplifier power supply =
and if a
zener diode is included in this line, this scheme may be satisfactory. =
However,
measurements on channel separation and harmonic and i.m. distortion, =
with
identical amplifier systems invariably show some advantage, =
particularly at the
low-frequency end of the audible spectrum, in the use of a separate =
power
supply for the pre -amp (even when the electrolytic bypass capacitors =
are still
new) and this arrangement is still recommended by the author as well =
worth the
small additional cost.
One point which has not been published, to the best of the author's
knowledge, concerns the particular advantage conferred by the feedback =
pair
amplifier using complementary transistors, such as that used in the =
low-pass
filter circuit, in comparison with the more usual n-p-n/n-p-n pair, =
where the
bias for the first transistor is derived from the h.t. line. In the =
case of the
n-p-n/p-n-p pair, any h.t. line feedback, due to inadequate h.t. line =
bypass,
will be negative rather than positive, and this can assist in obtaining =
good
t.h.d. figures down to low signal frequencies.
My thanks go to Malcolm Jenkins for providing the copy of the =
article=20
used to make this web page and to Lynn Miller for converting it into web =
format.
[ Back=20
to Index ]
HISTORY: Page created =
06/01/2002=20
13/01/2002 Hi-res Fig. 1 and December =
1970=20
postscript added
------=_NextPart_000_0000_01CF1844.9F58BF70
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