Norcim rc electronics club page 39......
David Caudrey takes a look at hobby electronics before the age of transistors.
A 459 MHz Valve Super-regenerative Model Aircraft Radio Control Receiver?
My co-author Terry
and I were into model aircraft at an early age. When I was at school, I thought
that to be able to control a model aeroplane by radio was the ultimate goal and
I read everything on the subject in the Aeromodeller
magazine. I understood little of what I read but it didn’t dampen my
enthusiasm. Certainly, I couldn’t afford the commercial gear which was
available at the time and if I was going to do radio control, I was going to
have to make it myself. (Terry probably got there well before me with the help
of the local radio repair man!)
Anyway freshly demobbed from National Service in the RAF, where I had learned a little about radio and electronics, I felt ready to have a go.
I purchased a cheap signal generator and made a simple 2kΏ/V multimeter and eventually I bought a simple absorption wavemeter suitable for 27MHz.
With this limited test gear I made a 27MHz transmitter (see page 8 of this site) and soft valve and hard valve receivers (see page 17 and others).
However, with no crystals, operation in the 27MHz band was less than ideal.
Only one model could fly in quite a wide area and a proclivity for the receivers to latch on to interfering signals caused problems. It was at this time that I learned that model control at 459MHz. was permitted and that it didn’t appear to be used. With the enthusiasm of youth, I naturally wondered if I could construct a 459MHz. system. I was aware of Lecher lines and the possibility of ‘measuring’ frequency with a ruler was certainly appealing.
The only available uhf. valve (tube) suited to low voltage battery operation was the 958A acorn valve and consequently an example was acquired from a government surplus dealer. I was aware that the 958A was specified for operation up to 350MHz. but this is in connection with its use as a transmitter valve, and I wondered if oscillation could be achieved at higher frequency but lower level, which would be ideal for a super-regenerative receiver. Of course, with little experience and without suitable test gear, I didn’t stand a chance but my curiosity about feasibility has never been lost.
Recently I discovered that the 958A is available from Vacuum Tubes Inc. of New Orleans and ordered an example. It was not expensive but packing and dues treble the cost in the U.K. The valve arrived promptly, new in the box which it was placed in April 1944.
Ad hoc holders for acorn valves are unobtainable so it was necessary to make something for installing what is an awkward component in a circuit. The result, which is shown in photographs below, employs the sockets from a B8G valve holder. It was not entirely satisfactory because, protruding below the mounting ring, it was too easy to dislodge the valve from the socket when the assembly was placed on the bench. This situation was improved by fitting the chubby ‘O’ ring as shown in the following photographs.
Having mounted the valve, I schemed out the circuit below and constructed it with what I had to hand in the way of contemporaneous components.
The schematic shows the basic UHF oscillator circuit with provision for inclusion of a controlling quench oscillator. Critical dimensions of the line are identical those of the passive line described in page 22 of https://davidcaudrey.me.uk with a target impedance of 330Ώ and velocity of 0.9c. However, this line differs in being suspended above an earth strip.
It can be seen from the photograph that
the line is extended to cover operation at 300MHz, the highest frequency which
I am able to display and measure currently; the brass object being the clamping
bar which determines the active length of the line.
When switched on and set for just below 300MHz squeg free sinusoidal oscillations were observed on the oscilloscope and the recorded frequency was 291MHz. Actual amplitude measurement was not tried because of the dc. potential on the line, the probe tip and its ground return lead being merely connected to form a pick-up loop. However, the oscillator was clearly doing what was expected of it.
So far so good, so the clamping bar was repositioned to define an oscillation frequency in the region of 600MHz. With no available means for measurement,
oscillation was confirmed by a simple absorption wavemeter as shown in the following photograph.
The wavemeter is Checker 1 which is untuned except that it has a helical aerial proportioned for 2.4GHz monitoring. A schematic for it is shown in Page 22 of this website. Checker 1 is the forerunner of Checker, 2 a version tuned to 2.4 GHz. shown in page 27. Happily, Checker 2 is blind to the emanation from the line!
Expenditure with respect to the purchase of a 500MHz oscilloscope certainly can’t be justified but an inexpensive frequency counter is certainly a possibility.
However development to include an integral quench oscillator will be a target.
If this is successful the Lecher line will be replaced by a compact tuned LC circuit and means for the detection of a 100% modulated incoming signal with be developed. The latter probably will involve an additional valve or contemporaneous transistor.
To produce super-regenerative receiver circuit a quench oscillator will be required, and the following figure indicates a likely circuit configuration :-
The obtention of a frequency counter permitted confirmation of the line parameters and a frequency of approximately 345 MHz was recorded, as shown in the following picture.
The quench coils are
apparent in the photograph but of course they are disconnected for frequency
The capability of non-intrusive frequency measurement permitted an assessment of the Lecher line parameters to be made and consequently the shorting bar was repositioned to give an indication of 300MHz.
The line length for this indication was found to be 22.5mm which corresponds with the expected propagation velocity of 0.9c.
It is reasonable to assume therefore that the line impedance is close to the target 330 Ώ.
oscillator coils depicted in the development schematic and in the photograph
are of the type employed in 27Mhz. receivers of the 1950s, typified by the Ivy
and Hill receivers mention in Page 17 of this site, i.e. 3mm wide pancake
windings between Paxolin or plywood discs held together with a brass
It was soon apparent that these were unsuited to use in the convenient cathode driven Clapp type circuit shown because of inadequate interwinding coupling and that a more conventional anode driven oscillator configuration would be need to be employed.
For the record the basic parameters are: -
Primary 650 turns
Secondary 600 turns (wire broke!)
Primary Inductance 4.2mH
Secondary Inductance 2.9mH
Primary Resistance 43 Ώ.
Secondary Resistance 35 Ώ.
The total series inductance (primary plus secondary) was found to be 8.25mH
which indicates that the coupling factor between windings is less than 20%.
(Perhaps it would be greater with a steel clamping screw!)
There maybe some addition to this page in the future. But Thanks for reading.