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One-Transistor
Radio This is
my version of a one-transistor radio that drives a speaker to
room-filling
volume and has very good selectivity and sensitivity without an outdoor
antenna. The
project came about after seeing Tom Polk's website "The
Macrohenrydyne" and his statement about it
being the "Most Powerful
One-Transistor Radio". This looked like a
challenge, so I set about
to design a better, or more powerful version of his circuit. The
following are the results of that quest: Tom's
"Macrohenrydyne" is a refined version of earlier circuits of Robert
Bazian and Charles
Wenzel Before
I begin, I want to thank Tom Polk for his expertise on the circuit and
Charles
Wenzel for not only advice, but for generously providing some of the
critical
parts of the project. Both of these
gentlemen were willing to share their knowledge and time without asking
for any
compensation. Also, I want to point out
that the project present here, is in no way representative of a better
or more
improved circuit than was previously published by the folks mentioned
above. The following project merely
documents my attempt to improve the design. My
final circuit is, in my
opinion, at least as good as my
predecessors. However, without actually
doing a
side-by-side comparison, it is impossible to tell which design is
better. I have determined, after all my experiments, that it is
really hard to get any more performance out of this type of
circuit. Regardless, I had fun with this
project, and the results
are
simply amazing! I only wish I had the parts and
this circuit when I was a kid. Back then, I thought a two
transistor "boy's" radio was super. This set easily outperforms
these! The final circuit represented
below, is a combination reflex and regenerative receiver. To
briefly describe the operation: The signal is tuned in with the primary
coil on the ferrite rod and variable capacitor combination. This
signal is loosely coupled to the base of the transistor where it (RF)
is amplified. At the same time, part of this signal is fed back
into the ferrite rod where it is amplified several more times,
comprising a traditional regenerative circuit. From
the diagram, It is not apparent how regeneration takes place.
This is accomplished by mounting T2 in close approximation to the
ferrite antenna bar to provide the correct amount of feedback.
The amplified (RF) signal is coupled through T2 to the detector diode
where the audio is recovered. Note that the diode also passes a
DC bias current, supplied by the 1 meg resistor, to the base of the
transistor. The .01 mfd capacitor removes any remaining RF so
that audio is also presented to the base where it is simutainously
amplified, along with the RF, by the transistor. This is the
reflex action. Finally, the amplified audio appears across T1 and
is coupled and impedance matched to the 8 ohm speaker. The reflex
action and regeneration is controlled, at the same time, by the pot in
the emitter circuit.
My
first attempt at making improvements, was a double-tuned circuit where
the collector, as well
as
the
ferrite bar antenna, were tuned together. It
looked good on paper, but in real life, it proved
impossible to make
the two circuits track. It appears that
with a regenerative circuit, the selectivity is so sharp, that
tracking can
only be accomplished with the absolute best-matched components.
Even with a precision dual-section variable
capacitor, a matching variable inductor and trimmer capacitors, I could
only
manage to make it track over about a third of the dial. However,
the part that did track, worked
amazingly well. If you wanted to make a simple, single station
radio, this would be practical. You could just use two trimmer
capacitors. Maybe I will post that circuit someday...
Closeup of the "Pacent"
variable capacitor After
going back to a single-tuned circuit, one thing became apparent, the
so-called
"Straight-Line" variable capacitors of later vintage were, in fact,
not that straight. They tended to crowd
the upper portion of the dial. The
solution was to use an old stock 1920's style, straight-line
capacitor.
The one I chose is an all-brass Pacent that
is about 365 picofarad. With the
Pacent, the center of the dial came out to 1100 kHz. as compared to the
more
modern capacitor, which placed it at 950 kHz. This
provided a dial, which was very evenly distributed
over its entire
length.
Rear view In
reference to Tom Polk's circuit, he used a Contra-Wound ferrite antenna
with a
switch that divided the broadcast band into two segments.
This resulted in spreading out the band in
two sections over the length of a slide-rule dial.
After experimenting with the Pacent capacitor and using a
14 to 1
tuning wheel, I decided to use a single space-wound ferrite bar and
spread the
whole band over one section of a similar slide-rule dial.
This still gave a resolution of about 1/16
inch per kHz. which is plenty for Dxing. The
ferrite bar, I used, is one that was salvaged from an
old Zenith
Model 1000 TransOceanic Radio. This is
a flat bar, 8 1/2 inches long. On this,
I space-wound 58 turns of 15/44 Litz wire for the main, tuned circuit,
which came out to 235 microhenries. This was followed
by 2 turns for the coupling winding. Here,
4 turns gave much more sensitivity, but a reduction
in
selectivity. 2 turns is a good
compromise. With this ferrite bar and variable capacitor
combination, the low end of the band started at 520 kHz. I
set the high end to 1710 kHz. with the trimmer capacitor that is in
parallel with the main variable. Left side Another
difference between Tom's circuit and mine, is the method of controlling
regeneration. He added a
feedback winding to the ferrite bar and with a combination of a
variable
capacitor and variable resistor, he was able to obtain smooth
regeneration. After trying his circuit,
which does work
very well, I noticed that there was a noticeable loss in power to the
output
transformer through the variable resistor. Also,
this design makes it necessary to have an additional
control on
the front panel. I thought if I could
eliminate the variable resistor, I could increase the speaker volume
somewhat. One method I tried, was
controlling the gain with a variable resistor across the coupling
winding on
the ferrite antenna. This, in effect,
shunts the signal that is applied to the base of the transistor. Although this works, it seemed to reduce the
"Q" of the ferrite bar antenna circuit when it was set at low
resistance, thus reducing the selectivity. This
method is used in both Robert Bazian and Charles
Wenzel's
designs. Another method is to place a
variable resistor in the emitter circuit to control the gain. This was a method used in older designs, one
of which is presented on Charles Wenzel's website.
With this method, there was negligible loss of power to
the
output transformer since the value of the resistor is very low. Also, since the resistor is in the emitter
circuit, there is no loading of the ferrite antenna circuit and no loss
of
selectivity. I used a 100 ohm, ten-turn
pot to provide a very smooth gain control. I
mounted it next to the circuit board and used a fiberglass shaft to the
knob so that there would be no hand capacity effects. The
ten-turn pot is not necessary, I just happen to have
it. A single-turn pot will work nicely. I
placed a 180 ohm fixed resistor
across the
pot to limit the minimum gain to the point where a high-power local
station
could be attenuated to a good listening level. With this setup,
the one control varies both regeneration and volume (reflex action). Closeup of the
circuit board Most of the circuit was built on a 2" x 2" piece of perf
board. T2 (black rectangle) is
an ISDN type of transformer that passes RF in the broadcast band of
frequencies
and rejects audio frequencies. I used a
FIL-MAG part # 66Z3088A that I had in my junk box.
Both Charles Wenzel and Tom Polk also used a commercial
transformer part # PE-64934. Charles
generously gave me a couple of these to try in my set.
In comparison, I was able to get more volume
at a given gain setting, with my transformer. This
is probably because of the 2:1:1 winding ratio that I
wired in
series for the primary. Regardless,
this increase in gain can be made up with a lower resistance setting of
the
gain pot. This
transformer is physically larger than what Charles and Tom used.
As I mentioned earlier, the regeneration is determined by the placement
of T2 in reference to the ferrite bar. In order to optimize the
placement, I mounted the circuit board to a 2 inch square piece
of Garolite, then with double-sided tape, I placed the board in the
correct location and stuck it to the base. I chose a location
that set
the feedback just under oscillation while having the gain control set
to maximum. If you are not able
to obtain proper regeneration, reverse the connections at points "C"
and "D". This will reverse the phase of the signal in
reference to feedback. The glass part, to the right of the
transformer, is the .22 mfd. capacitor. I tried a number of different
transistors, including darlingtons, in this circuit. Several were
generously supplied for comparison by Charles. Although many
worked, either with or without a change in bias, the MPSA18, which was
in the original design, always seemed to edge out the others in gain
and stability. I used socket pins on the circuit board for the
transistor and diode to make change-out quick. Some of
the circuits presented by Robert Bazian and Charles Wenzel used a
1N5711
Schottky diode for the detector. I have
tried this diode, and although it does increase the volume somewhat, it
distorts the audio noticeably. So,
I
used a 1N34 for the better fidelity. Right side The
audio output transformer (bottom left) is a common 70 volt line
transformer as used
in PA systems. I used the 4 watt tap on
the secondary to
drive the speaker. I brought the speaker audio out with a 1/4
inch phone jack (below the transformer). Although
the supply voltage indicated is 18 volts, the set performs almost as
well on
supplies as low as 8 volts. So, for a smaller version, a 9 volt
battery is sufficient. Battery drain is very low, in fact, when I
accidentally left the power switch on for over a week with the speaker
disconnected, the batteries were still in good shape when I found
it. Plus, they are just common carbon-zinc, not alkaline. The only other changes in the circuit were the values of the
decoupling capacitors, which also improved the
performance
somewhat. The dial scale can be made by first measuring the available
area then, in a CAD drawing program. draw and print out a graduated
scale with 1/10 or so increments, numbered sequentially. This will be your calibration scale.
Temporarily attach it to the dial then, with a signal generator, mark
every 10 kHz. across the whole dial. You can now remove it and
transfer the numbering to the drawing, fill in the 1 kHz. markers then
delete the calibration scale. After printing it out, attach it to
the front with either paper glue or double-sided tape. My scale
was drawn in Corel Draw and turned out to have 1/16 inch spacing
between each kHz. I used 1/4 inch Garolite for the base and front panel.
The dial pointer slide and ferrite bar holders (white material) are
high density polyethylene. Finally, to operate the set, turn the gain control fully
clockwise (least resistance), tune in a station then reduce the gain
until the distortion is eliminated. Further reducing the gain
will
set the volume. Since the ferrite bar antenna is very
directional, you can rotate the
set to bring in DX and also to null out strong local stations then
receive distance ones just 10 kHz. away! You can improve the performance by just adding a ground
connection to the common ground on the diagram. Also, an outside
antenna could be added by coupling one turn to the ferrite bar.
You might have to readjust the trimmer to keep the dial tracking since
this will load the tuned circuit slightly. However, I prefer to
use the set without any outside connections. This was a fun project and I have enjoyed several hours
logging many stations with this set. I plan on building more of
these marvelous radios. The next one will be a pocket version. Mike
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