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Vintage Radio
By Maurie Findlay, MIE Aust, VK2PW
Performance improvements for the
Hotpoint Bandmaster J35DE console radio
The two previous articles on this set dealt
with its restoration. The aim was to make
the set work as it did originally. We now
look at what can be done to improve the
performance in the light of design knowledge
some 60 years later.
I
F YOU ARE ONE of those who only
wish to restore a radio as close as
possible to the original, this article is
not for you. We can understand those
who strive to produce the vintage radio
equivalent of the Concours d’Elegance
but as we have pointed out in the past
when discussing many valve radios,
90 Silicon Chip
they often had design faults and unfortunate compromises.
OK, what was wrong with the design
of the Hotpoint? At the time it was
produced it would have been regarded
as a great set.
The most serious fault is the attenuation of higher audio frequencies due to
the tight selectivity of the intermediate
frequency stage. Selectivity refers to
the “sharpness” of tuning in a radio.
This was common to sets manufactured by big companies and built by
hobbyists in the 1940s and 1950s.
The usual practice was to have the
IF (intermediate frequency) at 455kHz
and one IF valve stage. Tuned transformers, each with two circuits, were
used, one between the mixer and the
IF amplifier and the other between the
IF amplifier and the diode detector.
Radios intended for use in country
areas sometimes had two IF amplifier
stages and three IF transformers – a
total of six circuits tuned to 455kHz.
They were great for picking up
distant stations but due to the severe
attenuation of the high audio frequencies, they always sounded very “mellow”. These days we would simply
regard the sound quality as muffled.
In order to appreciate why this happens, we need to look at the nature
of the signal transmitted by the radio
station.
Say the station is transmitting with
a carrier at 1MHz (1000kHz) and it is
modulated with a tone of 5kHz. Then,
the station is actually transmitting
three separate frequencies: 995kHz,
1000kHz and 1005kHz. If you put in
a filter which passes the 1000kHz but
attenuates the 995kHz and 1005kHz
frequencies, they will be reproduced
at a lower level.
Spectrum analysers and other sophisticated test instruments were not
generally available in design laboratories in the 1940s and 1950s and many
engineers were a bit hazy about the
idea of sidebands. In the 1960s, single
sideband (SSB) transmission became
siliconchip.com.au
Fig.1: while some vintage radio restorers may regard this as sacrilegious, this diagram shows how the circuit can be
modified to improve its performance. Specifically its audio bandwidth can be widened and the gain increased.
the standard for high-frequency communication circuits and designers
began to realise that you could survive
with one sideband only. But that’s
another story.
If people wanted a wider audio
response in the early years, the solution was to have a TRF (tuned radio
frequency) receiver. Many of these
were built by hobbyists from designs in
popular magazines. They usually had
three tuned circuits and two valve amplifying stages, followed by a detector.
The difficulty was that they were
only suitable for areas close to strong
stations. And if there were other stations close in frequency to the one
you wanted, they would often break
through. In other words, they had poor
selectivity.
A better solution
A better solution is to design the
455kHz amplifier so that it will pass
the higher frequency sidebands. How
high? Currently, in Australia, broadsiliconchip.com.au
Fig.2: this diagram shows how a top-coupling capacitor across the two coils
in an IF transformer can be used to increase the audio bandwidth.
cast stations are separated by 9kHz.
The authorities have taken great care
in allocating channels, in a geographical sense, so that there is little chance
of local interference from adjacent
channels. In theory, a filter which had
a level response centred on 455kHz
and maybe 20kHz wide would be OK.
But how to make such a filter? We
would have to get the old engineer’s
slide rule out and do some sums but
such a filter could easily have 16
inductors with precisely defined Q
factors. In addition, the losses through
the filter would certainly make it
necessary to have another amplifying
stage – not practical.
How about a compromise? There
is a way that the response to higher
audio frequencies can be improved.
It involves changing the coupling
between the windings of at least one
September 2011 91
The rather complex dial stringing arrangement which was pictured last
month is necessary to support the long pointer at top and bottom.
the 1st IF transformer improved the
audio response of the Hotpoint at 5kHz
by +6dB; a very worthwhile improvement for such a small modification.
How do you go about choosing the
best top-coupling capacitor in your
particular set? It’s a fiddly operation
but with care, the best value can be determined using only a multimeter. You
will have already peaked the IF coils.
Connect the multimeter to the test
point and carefully tune to a station,
preferably at the low-frequency end
of the band. Use an external aerial so
that the signal is reasonably strong and
not affected by body movements. The
meter should indicate -3V or more.
Next, solder a low-value capacitor (eg, 22pF) across the tops of the
IF transformer winding. There will
probably be a slight increase in the
meter reading.
Now try larger capacitors: 33, 47, 68
and 100pF in turn. One of these will
actually result in a lower meter reading and this is the correct one to use
to get the required over-coupling and
broader IF response shown in Fig.2.
Note that the IF tuning slug adjustments must not be altered
The value of capacitor for a given
degree of coupling could be calculated
if the inductance, the initial coupling
and Q factor of the IF transformer are
known but it is much easier to determine by experiment.
HT modification
Conveniently, the dial stringing arrangement is shown on the back of the dial
assembly itself. Without this diagram, it would be impossible to figure out the
dial cord path.
of the IF transformers. A little about
how coupled tuned circuits behave
will make the idea clearer.
The two windings on a 455kHz IF
are usually wound on a small diameter
former and placed in a shielded can
one above the other (see Fig.2). They
are each tuned by fixed capacitors
and a ferrite or iron-core slug which
can be moved up and down inside the
winding. The windings are carefully
placed so that when one is adjusted it
does not affect the other. This is called
under coupling and is how most IF
transformers are arranged.
If the windings are brought closer
together, the transfer of energy from the
primary to the secondary will increase
until a peak is reached. Bringing the
92 Silicon Chip
windings closer still then actually
reduces the energy transferred at the
455kHz centre frequency and boosts
the response on either side. This is
illustrated in Fig.2 with the curve la
belled “Over Coupled” and gives a clue
as to how the response can be widened.
Top coupling
It would not be easy to increase the
coupling between the windings by
moving them in an existing set but
the same result can be achieved by
connecting a small capacitor between
the tops of the windings. The degree of
over-coupling depends on the value of
the capacitor and we have done some
practical work to see what can be done.
A 47pF capacitor connected across
A slight complication now arises:
the hum on the high-tension (HT) line
is now applied to the grid of the IF
amplifier and the AGC-detector lines
via the top coupling capacitor. This
makes it necessary to put in a resistor/
capacitor filter to feed the high-tension
to the plate of the mixer valve.
The primary winding of the second
IF transformer will usually have a
high Q which will fill in the dip in
the response of the over-coupled first
IF but in our case it also contributed
to the sideband attenuation. A 0.1MΩ
resistor wired across the primary gave
the optimum overall IF response.
The improvement is well worthwhile and the resulting overall frequency response of the set is about
-3dB down at 5kHz instead of the
original -10dB (if you want the original
“mellow” tone, the function switch is
still available).
The modification makes it easier to
understand speech and enjoy music.
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September
August2011 93
2011
1
One curiosity of the Hotpoint J36DE set is that the loudspeaker is installed with
10mm spacers between its frame and the baffle. We’re not sure why this is so
but suspect that it was done to reduce the bass response because the set does
have audible hum. Alternatively, the designers may have been concerned about
acoustic feedback. As a consequence of this odd installation method, the entire
speaker cone had come away from the speaker frame and had to be glued back
in place.
However, it certainly does not make
the set comparable with modern FM or
digital receivers in terms of distortion
or frequency response.
Modifying the converter
Another quirk of the original design
of the Hotpoint is the operating condition for the 6J8G frequency converter.
The negative bias applied to the signal
grid is that supplied by the back-bias
resistor, through the AGC network,
plus that developed across the 200Ω
resistor at the cathode. It is too high.
As a result, the gain available for
weak signals is less than the valve
can provide.
The solution is to earth the cathode
of the 6J8G. This provides maximum
gain from the converter and better
operation of the oscillator, particularly
on shortwave reception.
With the cathode of the 6J8G
earthed, it is necessary to return the
shortwave aerial coil to the back bias
network. The added components are
a 1MΩ resistor and .047µF (47nF) capacitor. This retains the original idea of
no AGC on the converter on shortwave.
The overall gain of the set with the
modifications shown on the circuit is
actually slightly more than with the
original design. The increased mixer
gain and that attributable to the closer
1st IF coupling more than makes up
for the losses due to the damping of
the 2nd IF.
Even with the increased gain, the
Hotpoint needs a reasonable length of
internal or external aerial wire for good
daytime reception of local stations. All
glass miniature valves which became
available a few years later had much
higher gain. In combination with efficient ferrite rod aerials, they made
external aerials unnecessary for the
medium-wave band.
The original design also has a series 455kHz tuned circuit across the
primary of the broadcast aerial coil.
It was intended to reduce interference
from airport navigational beacons.
Unfortunately, it also reduces the
sensitivity of the radio, particularly at
the low-frequency end of the band and
when a short aerial is used.
Beacons of all sort are now kept
away from 455kHz so this filter is no
longer necessary. It can be disabled
by removing the associated 50pF
capacitor.
The set works better when modified
as described. It would be interesting to
talk to the set’s original engineer but
he or she has now probably passed on
to a higher design laboratory.
Increasing the audio power
Finally, the conservative operating conditions for the 6V6GT output
valve are worthy of comment. A 325Ω
cathode bias resistor is used with
about 250V applied to both plate and
screen. The optimum load for these
conditions is about 7000Ω and the
undistorted power output around 1W
at the speaker transformer secondary
(the original specification says 3W!).
Slightly more audio power can be
obtained by reducing the cathode bias
resistor to 250Ω and the plate load
to 5000Ω but at the expense of more
heat and shorter valve life. Speakers
used with sets of the period were quite
sensitive and 1W is enough for most
SC
situations.
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