In 2011, designing a frequency converter circuit consists in most cases of picking out an IC that has the
characteristics you need from a gain and mixer spurious product standpoint, add a couple filters, and a power
supply. In many cases the oscillator is part of the IC. Of course there are special cases where you have to use a
basic mixer and do everything yourself, but even that is simpler than designing a tube circuit. It really is
amazing what engineers and hobbyists of yore were able to accomplish using point-to-point wiring and a slide rule.
of Contents]These articles are scanned and OCRed from old editions of the
ARRL's QST magazine. Here is a list of the
QST articles I have already posted. As time permits, I will
be glad to scan articles for you. All copyrights (if any) are hereby acknowledged.
Here is a good article form the February 1941 QST magazine that discusses some of the considerations. Maybe you
have an old radio that this knowledge will apply to.
See all available
vintage QST articles.
Practical Design of Mixer Converter Circuits
Comparison of Tube Types and Checking Performance
R. Hammond (W9PKW)
THE design of an efficient mixer or
converter circuit is often the one thing that prevents the amateur from building his own communications receiver.
In application the amateur usually is unable to tell whether or not the stage is giving normal performance and,
lacking equipment for checking gain, no attempt is made to find out if it is doing the job efficiently. However,
there are simple ways of determining whether or not a mixer or converter is operating efficiently, and it is the
purpose of this discussion to explain these methods and to give some theory on the operation of converters. The
general characteristics of the several mixers and converters now available are also given, with a general
discussion of the performance characteristics of each.
An elaborate mathematical theory of the operation
of a converter or mixer1 is of no great importance for our particular problems. Roughly, a converter
operates as follows: Within the tube there is developed a current at oscillator frequency which is modulated by
the incoming signal to produce an intermediate frequency. The ability of the tube to develop a current at an
intermediate frequency is given by the" conversion conductance," which by definition is the ratio of an
incremental change in intermediate frequency current to the incremental change in r.f. signal voltage that
produces the current. This conductance in micromhos is published for all converters, and its use to calculate
stage gain is analogous to the use of mutual conductance with r.f. amplifiers. The gain equation for a single
tuned load is
where Gc is the conversion conductance, Rp is the plate resistance, and RL is
the tuned load resistance. Published values of plate resistance and conversion conductance can therefore be used
to calculate conversion gain. The tabulation following gives a comparison of gain for a group of tubes now
generally available. The gain figures were calculated for a tuned load impedance of 200,000 ohms, which is
equivalent to the better transformers now available.
If gain was the only consideration the above would suffice for the selection of a converter tube. Tube noise is
generally not a consideration when comparing converters simply because the converter is inherently a noisy device
and most converters develop noise voltages of approximately the same magnitude. The noise output of converters of
the 6A8 and 6SA7 type is approximately 4 times greater than that of an r.f. amplifier like the 6SK7 or 6K7. Where
the ultimate in signal-to-noise ratio is desired it is necessary to precede converters of this type with an r.f.
stage. Usually the selection of a converter is based on the characteristics of oscillator stability with regard to
a.v.c. and terminal voltage fluctuation, pull-in characteristics, oscillator transconductance that determines the
ease of oscillation especially at high frequencies, and other deleterious characteristics that cause loss in
performance at certain frequencies. The chart on page 41 indicates some of the characteristics of the various
converters. The gain figures and notes on stability and oscillator transconductance are of particular importance.
In general the converters perform equally well as mixers or as converters with the exception of the one
characteristic of oscillator stability. Any of the converter tubes gives good stability if used with a separate
oscillator and the circuits are isolated properly. Of the group the 6SA7 makes the best mixer because it gives
high gain and has improved internal shielding of the signal and oscillator grids. The improved shielding is
accomplished by using
What's the best mixer tube? How can a mixer circuit be tested to find out if it's doing the best job it can?
Here are the answers - plus design information of highly practical value.
shielding plates similar to the beam-forming plates used in beam power tubes. These plates are attached to the
side rods of the screen grid and confine the electron currents to beams which get into the outer regions of the
tube where they are modulated by the signal grid. The sketch of Fig. 1 shows the construction of the 6SA7. The
side rods of the No.3 or signal grid are mounted so that they split the' beam and make the electrons travel in
radial paths. Electrons turned back by the signal grid because of a strong r.f. voltage do not return to the
oscillator or No. 1 grid because they are caught by the collector plates. This reduces coupling between the signal
and oscillator grids and improves stability. Simple structures of cylindrical grids such as used in the 6L7 and
6A8 do not have this additional isolation and are therefore not quite as good as the 6SA7. The improvement in
stability evidences itself in the form of greater freedom from "pull-in " - that is, shifting of the oscillator
frequency with signalgrid tuning or with a strong signal on the signal grid. This effect is usually not as
serious as frequency shift due to terminal voltage fluctuation. The remarks relative to stability, given in the
tabulation on page 41, refer to the stability with regard to terminal-voltage fluctuation.
Typical circuits for the six converters listed in the tabulation are shown in
Figs. 2 to 7 inclusive. The 1A7G, 1R5, 6K8, 6A8, and 6SA7 can be used with separate oscillators simply by
connecting the oscillator grid of the converter to the oscillator grid of the oscillator tube. The screen and
other positive electrodes should be maintained at their normal rated d.c. voltages but should be by-passed to
Fig. 2 shows connections for a converter circuit using the 1A7G and Fig. 3 shows connections for
the 1R5. The 1R5 is one of the new miniature tubes for hearing aids and small portable receivers. The 1A7G has the
conventional 6A8 construction, using an anode for feedback. The chart above indicates that the gain obtainable
with either tube is approximately 34. The oscillator transconductance of the 1R5 is slightly higher and the
oscillator stability is somewhat better. These two features are of advantage for high frequencies.
Figs. 4, 5, 6 and 7 show connections for converter circuits with types 6A8, 6K8, 6J8G and 6SA7
respectively. The high oscillator transconductances of the 6K8 and 6SA7 make them particularly suited for
all-around usage. They oscillate strongly at high frequencies where Lie ratios are unfavorable. The 6A8
construction is not satisfactory for amateur usage because of instability in the oscillator. The oscillator
electrode is a pair of rods located in the tube between the No.1 grid and the screen. These side rods collect
electrons from the cathode stream and the electrode current is controlled by the No.1 grid. Unfortunately,
changes in signal-grid or screen voltage also change the anode current. This conductance between signal grid and
oscillator causes instability with variation in a.v.c, voltage. Fluctuations in screen voltage due to supply
regulation also change the frequency. As a result, the 6A8 is subject to motorboating or "put-put" at high
frequencies. Dial calibrations also drift with line voltage fluctuations. "Pull-in" is particularly bad with the
The 6J8G construction incorporates a triode oscillator and a mixer section with a common cathode.
This construction results in good stability insofar as screen and a.v.c. voltages are concerned. The 6J8G has two
serious disadvantages, however, that have limited its application. The triode section shares a portion of the
cathode area. The area used by the triode is quite small and as a result the oscillator transconductance cannot be
made high. Also, at high frequencies a peculiar effect is experienced that causes a flow of current to the signal
grid. This current causes a high negative potential across the resistance in the grid return, and this bias
reduces the gain of the mixer. The effect can be reduced somewhat by using a high value of screen voltage, but it
is then necessary to increase the bias to hold the cathode current to a safe value.
The 6K8 has been used extensively by the amateur and also the commercial manufacturer principally because it gives
fair stability, and design problems are usually simple. The tuned-grid oscillator shown in Fig. 5 gives very
little trouble and is easy to build. The oscillator frequency is not independent of screen and .v.c. voltages, but
in most designs the frequency shift caused by one is offset by the other so that good stability is obtained. The
6K8 has an effect known as spacecharge coupling which is experienced at high frequencies. This effect is as
follows: The oscillator voltage on the No.1 grid causes a fluctuation in the number of electrons in the region of
the signal grid. The electron density changes at the oscillator frequency and as a result a displacement current
flows into the signal grid. At high frequencies where the signal grid and oscillator frequencies are quite close,
the impedance of the signal grid circuit at the oscillator frequency is quite high and as a result the
displacement current produces an a.c. voltage across the signal grid circuit. This voltage, when smaller than the
bias, reduces the gain of the tube slightly. Under extreme conditions it overrides the bias and causes
rectification in the signal-grid circuit, causing a serious loss in gain. The coupling can be neutralized by a
small capacitance - approximately 2 or 3 μμfd - between oscillator and signal grids. Commercial practice is to use
a condenser (known as a "gimmick") made by wrapping two pieces of wire together to give the desired capacitance.
Neutralizing the space charge increases the gain and image ratio.
Fig. 2 - Converter circuit for the 1A7G or 1A7GT.
Fig. 3 - The 1R5 converter circuit.
Fig. 4 - Converter circuit for use with the 6A8. 6A8G or 6A8GT.
Fig. 5 - The 6K8, 6K8G or 6K8GT converter.
Fig. 6 - Converter circuit for the 6J8G.
Fig. 7 - The 6SA 7 converter circuit.
Fig. 1 - Diagram of the 6SA7 structure, showing electron beams.
The 6SA7 construction has already been described. Using cathode feedback in the Hartley circuit shown in Fig.
7, excellent stability is obtained. The gain is quite high and the high oscillator transconductance makes a good
The 6SA7 converter is tricky to use because the cathode returns through the oscillator coil. This
connection, however, is the secret of the stability resulting with the 6SA7. The feedback is obtained from the
total cathode current. A.v.c. voltage variations on the signal grid do not change the cathode current appreciably
so that the oscillator frequency is almost independent of a.v.c. Screenvoltage variation produces a shift in
frequency in the opposite direction and the two effects practically cancel. The frequency change with either
variable is reduced by using the optimum tap on the oscillator coil. With average oscillator coils the tap should
be adjusted to give a total oscillator voltage of approximately 10 volts grid-to-ground. Under these conditions
the oscillator grid current measured in the grid leak will be approximately 0.5 milliampere. This current can be
measured with a 0 to 1 milliammeter by connecting it at the bottom of the grid leak.
At high frequencies
it is necessary to keep the leads connecting the cathode to the coil, and the bottom of the coil to ground, as
short as possible. The cathode lead in particular should be short. The inductance of this lead is not a part of
the oscillator tank and oscillator voltage developed across it does not contribute to feedback. The voltage does
bias the signal grid, however, and will reduce the gain of the converter. Under extreme conditions the voltage may
be high enough to cause a flow of current in the signal-grid circuit. This current results because of high voltage
between cathode and ground and because of phase shift of this voltage with respect to the voltage between grid and
cathode on the coil. The cathode connection to the coil should also be made so that the lead pulls away from the
coil at right angles. By pulling the wire away parallel to the winding the cathode-lead inductance may cancel a
portion of the tap-to-ground inductance.
In band switching arrangements the circuit of Fig. 8 is
recommended. It will be noted that the tap switch on the oscillator coil is located at the ground end of the coil.
This puts the inductance of the switch and its connecting leads within the closed tank circuit. Since the tank
currents flow through this inductance it contributes to feedback and gives oscillation with a minimum of
cathode-to-ground voltage. If the switch was between the cathode and the coil in the position of lead 1 the drop
across the switch inductance would not contribute to oscillation, but would produce a high cathode-to-ground
voltage. As mentioned above, this voltage is shifted in phase from the voltage in the tapped portion of the coil
and may cause the signal grid to be driven positive and cause rectification.
The circuit of Fig. 9 shows
the 6SA7 as a mixer. It will be noted that the neutralizing condenser Cn. is used to neutralize the
space charge. The 6SA7 as a mixer gives an increase in gain over that realized as a converter.
Space-charge coupling is also experienced with the 6SA7, and a "gimmick" is required for neutralization. This
coupling is characteristic of converter or mixer systems wherein the oscillator voltage is injected next to the
cathode or filament. The 6J8G, although not having this coupling, has the transit-time effect which is just as bad
and cannot be neutralized. The transit time effect is experienced with converters or mixers in which the
oscillator voltage is mixed in the cathode stream outside of the signal-grid injection.
* Circuits using both plate and screen current for feedback can be employed and the
effective transconductance is then 1200 micromhos.
** Transconductance in micromhos at rated conditions. Note
- Gain figures are relative for a tuned load resistance of 200,000 ohms.
It might be of interest at
this point to give the accepted theory on what causes the transit time effect. Electrons accelerated through the
No.2 screen grid approach the No. 3 injector grid. At high frequencies, where the time of transit between cathode
and No.3 grid is an appreciable portion of the period of oscillation, electrons accelerated by the No.3 grid on
its positive swings reach the grid at a time when it is going negative and are repelled and turned back toward the
screen. On the way back they are accelerated by the positive potential on the screen and by the increasing
negative potential of the No.3 grid. Many of these returning electrons reach the screen and are drawn off as
additional screen current. Some of the electrons, however, pass very close to the screen and are accelerated
toward the No. 1 grid at high velocity; many of them obtain sufficient energy to overcome the negative potential
of the No. 1 grid and flow in the external No. 1 grid circuit. This flow of current is d.c., and in a direction
such that the drop in the external resistance increases the bias. If the tube is operated from the a.v.c. string
as in the conventional case, the total return to ground is of the order of two megohms. A current of several
microamperes increases the bias sufficiently to cause an appreciable loss in gain. The current can be eliminated
for frequencies up to approximately eighteen megacycles by increasing the bias and the screen voltage.
Fig. 8 - Recommended oscillator switching for the 6SA7.
Fig. 9 - The 6SA 7 mixer, separately excited by a 6J5 or 6J5G oscillator.
Fig. 10 - Circuit for making performance tests on the 6SA 7 converter.
Fig. 11 - Triode mixer with separate oscillator.
The above information should be useful in determining the converter
to be used for a particular job. Once the converter is built it is comparatively easy to ascertain whether
performance is satisfactory. Of course in the laboratory the most satisfactory method is to check stage gain with
a signal generator, but few of us have signal generators with which to make precision measurements. We usually
rely on the sound of the set and whether it pulls in the signals.
The first check on any converter is to
measure the electrode voltages with a high-resistance meter. The correct voltages are indicated for the various
circuits. Next in order of importance is to check to see if the oscillator amplitude is high enough. The easiest
method of checking this is to measure the d.c. grid current in the grid leak. This grid current increases directly
with oscillator voltage and is so closely related to oscillator voltage that manufacturers, instead of rating the
oscillator voltage to be used with a converter, rate the grid current as measured in a recommended grid leak. On
each of the preceding circuits the rated oscillator grid current is given. In practice the grid current cannot be
held to this value over the band, especially if a wide tuning range is desired as in commercial broadcast sets. In
communications receivers where the tuning range is small the variation is not large. A 2-to-1 variation in a set
having a wide tuning range is not bad. If rated grid current is obtained in the middle of the band the variation
over the band is usually not excessive. The grid current is important because it determines the point of optimum
gain, and other than rated value results in a sacrifice in performance.
Converters using the 6A8, 6K8,
6SA7, 1A7G, or IR5 should next be neutralized for space charge coupling. This is accomplished by connecting a
"gimmick" between the oscillator and signal grids. If a gang condenser is used and the oscillator and signal grid
sections are adjacent, neutralization can be accomplished by connecting the "gimmick" between the stators of the
two sections. Commercial practice is to solder two small pieces of wire to the stator lugs and then to twist the
ends together. About two turns is satisfactory. Note: Neutralization is done on the highfrequency edge of the
highest-frequency band. Low-loss wire should be used. The capacitance should be adjusted to give maximum
There are several phenomena that can take place that will upset performance after the above
considerations have been observed. Parisitic oscillations take place in the oscillator section if too much
feedback is used or if the values of grid coupling condenser and grid leak are too high. A 50-μμfd grid condenser
is usually satisfactory for most circuits. Most grid-leak specifications call for 50,000 ohms. Battery tubes
having low oscillator mutual are specified with as high as 200,000 ohms, and the 6SA7 with its high oscillator
mutual or transconductance is rated with 20,000 ohms. If the oscillator and signal-grid circuits are not
adequately shielded and isolated, severe coupling between circuits is obtained at some frequencies. The
signal-grid circuit in extreme cases may load the oscillator enough to cause it to stop oscillating. This effect
can be detected by observing the oscillator grid current as the set is tuned through the coupling point. A rapid
dip in the oscillator grid current is experienced as the coupling point is passed. Shielding of coils and
isolation of parts and leads eliminates this trouble. Motorboating on strong signals is the result of oscillator
shift with a.v.c. and other element voltage variation. It was pointed out that the 6A8 was particularly bad in
this respect, that the 6K8 was much better, and that the 6J8G and·6SA7 are very good. Motorboating can be
experienced with the 6J8G and 6SA7 if powersupply regulation is bad and if the oscillator amplitude is not
adequate. Stability is improved by operating at or somewhat over rated amplitude.
The major troubles
experienced with converters produce a flow of grid current in the signal-grid return. This is true of the transit
time effect with the 6J8G, the space charge effect with 6K8, 6SA7, 6K8, 1A7G and 1R5, and the phase shift of the
high cathode to ground voltage in the 6SA7. The circuit of Fig. 10 shows how a check for signal-grid current can
be made without the use of a sensitive microammeter. An electron-ray indicator tube such as the 6U5/6G5 will
indicate any current flow in the a.v.c. return. Most returns have about three megohms total and a d.c. current of
1 microampere will produce 3 volts, which will make a noticeable deflection on the target. The voltage drop
between the bottom end of the coil and ground should never exceed approximately 1.5 volts. This voltage can exist
because of contact potential in the diode and other grids connected to the a.v.c. system, and does not indicate
Signal grid current with the 6A8, 6K8, and 1A7G usually results from space-charge coupling, as
already described. A convenient test for its presence is to short the signal-grid tuned circuit with a condenser.
This shorts out the voltage and eliminates the current. 'The "gimmick" when adjusted properly neutralizes space
Signal-grid current because of space-charge coupling is also obtained with the 6SA7 but
in addition current can flow because of high cathodeto-ground voltage and phase shift of this voltage with
respect to the oscillator grid-to-cathode voltage. If bypassing the signal grid does not eliminate the current,
the trouble will be found in the oscillator coil and connecting leads. The cathode lead should be kept short and
the circuit of Fig. 8 adhered to. The ratio of length to diameter of the oscillator coil should not exceed more
than about 1.5 to 1. With long coils and small diameters there is appreciable phase shift with attendant troubles.
As mentioned previously the cathode lead should pull away from the coil at right angles so that it does not couple
to the coil.
Recently, certain manufacturers have used triodes for mixers. A typical circuit for this type of mixer is
shown in Fig. 11. It will be recognized as similar to many of the circuits used in the older days. In commenting
on this circuit it might be said that the chief advantage of the triode is that it develops very little noise. It
is thus possible to add extra gain behind the converter in the i.f. and get high sensitivity with a good
signal-tonoise ratio. The triode in this connection has serious disadvantages, however. It is necessary to use a
special low-impedance primary i.f. transformer so that the grid-to-plate capacitance of the triode will not cause
loading of the signalgrid circuit. In the practical case the tuning condenser required to tune the i.f. primary
is approximately 2000 μμfd. The high cathode-togrid capacitance causes severe coupling of the oscillator and
signal-grid circuits. This evidences itself in the form of instability with a.v.c. variation, "pull-in " on strong
signals, and oscillator shift with tuning of the signal grid circuit. In applications where stability is not of
prime importance a pentode such as the 6SJ7 or 6AB7/ 1853 could be used to give good signal-to-noise ratio. The
low signal-grid-to-plate capacitance in these types would allow the use of conventional i.f. transformers.
* Ken-Rad Tube & Lamp Corporation, Owensboro, Kentucky.
1 In common terminology, a "converter" is a tube
performing the dual functions of mixer and oscillator; a "mixer" does not incorporate an oscillator section. Any
converter tube can be used as a plain mixer by providing excitation from a separate oscillator tube. - ED.
Posted 6/16/ 2011