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VINTAGE RADIO
By RODNEY CHAMPNESS, VK3UG
Intermediate Frequency (IF)
Amplifiers; Pt.2
Last month, we looked at how the IF stage
evolved in early broadcast-band AM radios.
This month, we look at high-fidelity IF
amplifier stages and describe how to get rid
of the 9/10kHz whistle.
P
RIOR TO THE introduction of
FM into Australia, some radio
manufacturers produced receivers that were capable of reproducing
the full transmitted audio bandwidth.
Typically, this involved designing
20kHz IF (intermediate frequency)
stages to give a maximum audio frequency response of 10kHz.
However, the use of a wide-bandwidth IF laid the receiver open to
annoying “monkey-chatter” – ie, distorted modulated audio signals from
stations close to the tuned frequency.
It also gave rise to annoying 10kHz
Fig.1: the circuit for a 9/10kHz
audio notch filter. It is designed
to filter out 9kHz or 10kHz
whistles (depending on the
station spacing) in a wideband
AM receiver.
84 Silicon Chip
heterodyne whistles from stations
on adjoining channels. The monkey
chatter couldn’t be eliminated but the
10kHz whistle could be and often was.
Basically, the 10kHz whistle was
“eliminated” by installing a simple
10kHz audio notch filter. This filter
effectively reduced the whistle to an
insignificant level.
The 10kHz filter often took the form
of a narrow-band rejection filter, as
shown in Fig.1. In this case, the filter is
physically tuned to 10kHz by varying
L1 or C1 and C2, while the depth of
the notch was adjusted by VR1. Note
that, with the advent of 9kHz channel
spacing, these filters had to be retuned
from 10kHz to 9kHz.
Variable selectivity IF stages
In most cases, broadband amplifiers did a good job on local stations
and gave an audio output which
was considered high-fidelity at the
time (10kHz compared to FM which
has frequencies as high as 15kHz).
However, listening to more distant
stations was often quite unpleasant
at night, due to fading, noise and interference, monkey chatter and 10kHz
heterodynes.
To counter these extremely annoying problems, most high-fidelity receivers included a switch that reduced
the IF amplifier bandwidth to around
10kHz. This meant that the receiver
could produce audio signals up to only
about 5kHz when the switch was in
the “narrow” position.
Fig.2: a variable bandwidth IF stage. Switching the
resistors across the IF transformer windings increased
the bandwidth, while reducing the gain of the
amplifier.
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This photo shows an assortment of 455kHz
IF transformers. They came in a wide range
of sizes.
Of course, this meant that the full
frequency range was no longer reproduced, so listeners had to be content
with less than “hifi” reproduction.
However, on the positive side, the
10kHz whistles, monkey chatter, noise
and interference were all signifi cantly
reduced. This was important because
before the advent of TV, the evening’s
entertainment often involved listening
to the radio.
Variable bandwidth
Taking this a step further, some
manufacturers designed variable
bandwidth IF stages that could be
switched to suit the listeners’ requirements. This was done in a variety of
ways.
One method involved switching
resistors across the IF transformer
windings. This lowered the Q of the
windings and the gain of the amplifier,
while at the same time increasing the
bandwidth of the amplifier – see Fig.2.
Another method involved removing
one IF transformer completely, replacing it with an untuned inductance-capacitance network.
Still another method involved
switching a tertiary winding in and out
of circuit in a special IF transformer.
There were even circuits which automatically adjusted the bandwidth
according to the strength of the received signal – ie, the bandwidth was
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controlled by the AGC.
However, although such circuits
were around, very few showed up in
the average domestic receiver. It’s also
interesting to note that specialised
high-fidelity tuners/receivers often
used an IF of 1900kHz (or some other
frequency above the broadcast band)
to achieve good bandpass shape and
20kHz bandwidth.
Unfortunately, fading – and selective fading in particular – remained as
a severe impediment to good quality
reception on distant stations. For those
unfamiliar with selective fading, it
manifests itself as severe distortion
and fading of the received signal. It is
usually due to multi-path reception,
which causes the relative levels and
phase of the carrier and its two side
bands to vary.
Keeping IF amplifiers stable
It is rare to have instability and oscillation problems in well-designed amplifier stages. By using an IF of 455kHz
and normal high-gain IF transformers,
a valve with a mutual conductance of
around 2000 was all that was necessary
to obtain the necessary performance.
Valves such as the 6U7G and the 6N8
fall into this category.
To ensure stability under all circumstances, it is necessary to make
sure that the layout of the amplifier is
such that inputs and outputs are kept
well apart. This particularly applies
if using high-gain valves. In some
cases, such as when using high-gain
valves like the 6BA6 (and more so
with the 6AU6), a shield may need to
be soldered across the valve socket,
isolating the input from the output.
As a matter of interest, I’ve found a
number of Healing sets using the 6AU6
to be marginally stable.
Neutralisation
Fig.3: this diagram shows the
correct positions for the slugs in
an IF transformer. Note that the
coils are tuned with the slugs
towards the outside ends of the
former (not in the centre).
Neutralisation was used in circuit
design back in the 1920s when triodes were used as RF amplifiers. It
was necessary if reasonable gain was
to be obtained without the amplifier
oscillating. However, with the advent
of RF tetrode and pentode valves,
January 2003 85
Fig.4: typical IF, detector and audio stages for an AM broadcast band receiver. The components marked with an
“A” suffix are often missing but their inclusion improves performance (see text).
neutralisation became unnecessary
in most circuits, particularly in IF
amplifiers with their relatively lower
frequency of operation compared to
RF amplifiers.
However, I’ve found that EMI/HMV
have been sticklers for doing things
right. Fig.4 shows a circuit in which
the IF stage is approximately neutralised. The 5pF (C2) capacitor from the
plate of the 6BA6 to the bottom of the
secondary of the IF transformer acts
with the AGC bypass (C1) to form a
bridge neutralising circuit.
I had a Little Nipper receiver to
restore some time back which had an
unstable IF amplifier – it tended to
oscillate if I wasn’t careful with the
alignment. It turned out that someone
had been at the set before it came to
me and had replaced the .01µF AGC
bypass capacitor (C1) with a value of
0.1µF. Replacing this capacitor with
the correct value restored the neutralisation and the IF stage was again
quite stable.
Detector & AGC leads
The leads from the detector and the
AGC diode tend to be treated as having
no RF energy on them. In reality, however, they carry quite a bit of RF (IF)
energy and this needs to be prevented
from radiating and causing instability
within the receiver.
For example, resistors R3 and R4
should have minimal lead length on
the ends connecting to pin 5 of the
6AV6. Similarly, the 47pF capacitor
86 Silicon Chip
(C7) lead from pin 5 of the 6BA6 should
be as short as possible, as should C5’s
lead on the IF transformer terminal. By
observing these precautions, minimal
IF energy will be radiated from the IF
amplifier circuits.
The detector lead to the volume
control can also radiate energy if it
isn’t shielded. However, few receivers
in the later valve radios have this lead
shielded so it isn’t always necessary.
Note too that some receivers have the
volume control di
rectly connected
to the bottom of the IF coil as shown
in Fig.4 (assuming that R2A is a wire
link). In that case, only the 100pF
bypass capacitor (C5) provides RF
filtering.
By contrast, the better receivers
include another section of filtering
based on resistor R2A and capacitor
C6A. This further reduces the level of
RF (IF) energy getting through to the
audio amplifier.
Although the audio amplifier favours audio frequencies, it also amplifies any IF signals that find their way
into this stage. This signal can then
be radiated from the audio amplifier
and picked up by the front-end of the
receiver, or by other receivers nearby, where it can cause some strange
effects.
In some cases, this radiation causes
the receiver to perform poorly at the
low-frequency end of the broadcast
band. It’s difficult to describe the
exact symptoms. However, the set
doesn’t have the sensitivity it should
and also seems to be a little strange in
its alignment, with a certain amount
of “swish” heard as the set is tuned
across a station.
So what can be done to overcome
this problem. The amount of IF signal
getting into the audio amplifier has
already been reduced by the filter consisting of R2A and C6A. In addition,
capacitor C8 from the plate of the 6AV6
to earth also reduces the amount of IF
energy in the circuit.
However, if the lead lengths from
the plate of the 6AV6 to the grid of the
6M5 are short, it would be better to
connect a small-value capacitor (such
as C11A) between the grid of the 6M5
and earth. The combination of R8 and
C11A would then be more effective at
reducing the IF energy applied to the
grid of the 6M5 than using just C8.
Most output stages have a capacitor from the plate to chassis or to the
high voltage supply. This reduces the
amount of IF energy at the output of
the audio amplifier, as well as acting
as a mild top-cut audio filter. The suggested added components that reduce
this problem are shown with an “A”
after them in Fig.4 (R2A is normally a
short circuit in most sets). By carrying
out these modifications, I’ve found
that many receivers offer improved
performance.
Another set I looked at some time
ago had an extremely unstable IF amplifier. It didn’t take long to establish
that RF signals were being amplified
in the audio stage and were being fed
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back through the set. In fact, it was so
unstable that even bringing the plastic
handle of a screwdriver near some of
the normal supply wiring caused the
set to either go into oscillation or to
stop oscillating, depending on the state
it was in at the time.
In this case, the problem was found
to be lack of proper filtering of the
high-tension (HT) supply line. In this
particular receiver (from a well-known
manufacturer), R9 was not includ
ed in the circuit design – there was
just a length of wire where a resistor
could (should) have been. I decided
to decouple the HT line by installing
a resistor in this location and the
set imme
diately became stable and
proved to be a really hot performer.
Problems can also occur when IF
cans are not earthed prop
erly or a
shield can is missing from a valve.
These are problems that are easily
fixed.
Despite a few problems, I have
generally found IF amplifi
ers to be
quite reliable. In most cases, all that is
necessary to restore the performance
is to replace leaky paper capacitors
and perhaps the odd valve. The AGC
bypass capacitor(s) are particu
larly
important and these should have no
discernible leakage. If they do, the
normal AGC control voltage will not
be applied and this usually results in
overloading of the IF amplifier.
An IF amplifier with low gain
It’s important that IF transformers
be wired the correct way, as reversing
the connections on one winding can
cause the gain to be quite low. Many
replacement IF transformers, such as
those produced by Aegis, have the
connections marked on the can, so
they are easy to identify.
For unmarked transformers (eg,
those salvaged from derelict receivers),
the windings can usually be identified
by taking the transformer out of its
shield can. The grid winding is the
one furthest from the base. If the performance is poor and you know the
transformer is good, try reversing the
connections. Also, if an IF transformer
is being taken out of a wreck, observe
what each lead is attached to and label
the leads accordingly.
The following information from the
4th edition of the Radiotron Designer’s
Handbook (by Langford-Smith) will
help in identifying IF transformer
windings: “For the capacitance and
mutual inductance coupling to be
aiding, the prim
ary and secondary
windings are arranged so that if the
plate connects to the start of the primary, then the grid (or diode plate) of
the next stage connects to the finish
of the secondary winding; both coils
being wound in the same direction . . .
the grid and plate connections should
be as far from one another as possible”.
Aligning the IF amplifier
The standard IF transformer usually has critical coupling between the
two tuned circuits. Critical coupling
provides maxi
mum gain with the
transformer adjusted by simply tuning
for a peak.
IF transformers employ a variety of
methods when it comes to adjusting
the slug-tuned types. Older types
have an earthed metal screw thread
which can be adjusted with a normal
metal screwdriver. Conversely, if the
tuning tool has to be inserted into the
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January 2003 87
Photo Gallery: Eclipse Monarch DKL
Manufactured by Eclipse Radio (Melbourne), the 1947 Monarch DKL is
a good example of the 4-valve reflex superhet designs that were popular
during that period. The set was available in a number of different cabinet
colours, including white as shown here. The following valves were used:
6A8-G frequency changer; 6B8-G IF amplifier/reflexed 1st audio/detector/
AVC amplifier; 6V6-GT output; and 5Y3-GT rectifier. (Photo and information
courtesy Historical Radio Society Of Australia).
IF transformer, you use a non-metallic
alignment tool.
It is also important to use the right
tool here for two reasons: (1) so that the
slugs are not damaged; and (2) so that
the transformer is not detuned by the
presence of a metallic adjustment tool.
Plastic alignment tool kits are available from various electronics stores or
you can use knitting needles which
have their ends filed to a screwdriver
blade shape.
The older type IF transformers that
use trimmer capacitors across the
tuned winding are also best adjusted
with a plastic alignment tool. That’s
because the plate voltage (ie, the HT)
is usually present on at least one trimmer – use a metal tool and you could
get a nasty shock.
The alignment procedure is as
follows: first, with the set turned off,
connect a digital multimeter (DMM)
across C1 on the AGC line and switch
to the 0-20V range. That done, connect a signal generator to the antenna
terminals of your set and tune the
set to the low-frequency end of the
broadcast band.
The next step is to apply a high-level
signal modulated at 1kHz at around
the expected IF frequency and tune
88 Silicon Chip
the generator across the band. If the
set hasn’t had its IF tuning adjustments
fiddled with, a response should be
heard at or near 455kHz (or what ever
the nominal IF of the set is).
If the signal through the set is quite
strong, the DMM will register an extra
-2V along the AGC line. Adjust the
output of the generator so that only
-1V or so of extra voltage is shown on
the meter.
If the frequency is some way away
from the expected IF (eg, 20-30kHz),
it is possible to “walk” the IF adjustments onto the required frequency. To
do this, first tune the signal generator
just to the side of the spot where the
maximum response is (ie, towards
the wanted frequency). That done,
adjust each of the IF slugs for a peak,
then go through the whole procedure
again until the maximum response is at
455kHz (if this is the target frequency).
Now it is necessary to accurately
tune the IF amplifier. Once again,
adjust the signal generator so that
the DMM reads a volt or so above the
standing bias on the AGC line. Adjust
each of the internal slugs or external
screws for a maximum reading on the
DMM, except for the tuned winding
going to the detector diode. This one,
at the top of the transformer, is adjusted for maximum audio, not maximum
meter reading.
If the DMM is connected across
the volume control (VR1), peak all
adjustments for a maximum reading.
Reduce the generator signal level if the
DMM reading is above about -4V, as
the IF amplifier tunes (peaks) slightly
differently with a strong signal compared to a weak signal. Note that for
best performance on weak signals, it
is necessary to align the set on weak
signals.
Note particularly that the slugs or
screws should adjust to the correct
frequency with the slugs and screws
away from the centre of the former,
as shown in Fig.3. If they are close
together (ie, towards the centre of the
former), the coupling between the two
tuned circuits will be upset and the
performance will be compromised.
If you don’t have a signal generator
it’s still possible to align the set, although not quite as accurately. Once
again the DMM is connected to either
the AGC line or to the detector output.
All you have to do then is tune to
a relatively weak sta
tion and peak
the signals as described in the previous paragraph. Of course, you won’t
know if the IF stage is tuned to exactly
455kHz but that doesn’t really matter.
Note that this job should be done in
the middle of the day, to avoid signal
fading which would make it difficult
to accurately align the IF amplifier.
So there you have it – a straightforward method of tuning the IF amplifier
stages in most sets. In times gone by,
when high impedance voltmeters were
scarce, the audio output was measured
and the IF adjustments peaked for
maximum audio. However, I believe
that the method I’ve described is more
appropriate today as it also gives an
idea as to whether the AGC system is
working as it should.
Occasionally, one slug in an IF
transformer will be stuck. If you strike
this, don’t force it as broken slugs are
hard to get out. Instead, just adjust
all the other slugs so that all tuned
circuits are on the same frequency as
the circuit that’s tuned by the stuck
slug. Being precisely on 455kHz isn’t
at all necessary.
Finally, for anyone who wants to
know more about IF amplifiers, take
a look at the relevant chapters in the
“Radiotron Designer’s Handbook” by
SC
Langford-Smith.
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