May 1957 Radio & TV News
These articles are scanned and OCRed from old editions of the Radio & Television News magazine. Here is a list of the Radio & Television
News articles I have already posted. All copyrights are hereby acknowledged.
It took me a couple passes of the explanation to comprehend the
advantage of a Thomson-Varley (aka Kelvin-Varley,
since Thomson and
Lord Kelvin are one and the same person) switchable voltage
divider compared to a standard type. At first I thought the author,
Edwin Bohr, was
implying that the source and load impedances would not have as great
of an effect on the accuracy of the divider (and to some extent
it is less sensitive), but the main advantage is that the configuration
permits simple cascading stages of decade dividers to achieve essentially
any degree of resolution. Both a standard series-wired type voltage
divider and the Thomson-Varley need ten resistors and eleven switch
positions to provide 10 equal steps (plus
bypass). However, using the same approach for 100 equal steps
in the standard divider scheme would require 100 resistors, 1000
steps would require 1000 resistors, etc. The Thomson-Varley divider
cascades decades of dividers so that 100 equal divisions requires
only 20 resistors, 1000 divisions requires 30 resistors, etc.
Such a 'breakthrough' idea was particularly significant in the days
when large radial lead components and multi-layered wafer switches
that were point-to-point hand-wired were all that were available,
as compared to printed circuit boards that are automatically assembled
with pick-and-place robots today. Obtaining large quantities of
precision resistors is a lot easier nowadays as well. Metrology
laboratories still use Thomson-Varley type voltage dividers for
Note: Edwin Bohr does do appear to be
a direct relation to physicist
Niels Bohr, although there certainly must be some familial tie.
An Accurate Voltage Divider
By Edwin Bohr
Ingenious wiring, using an inexpensive switch, enables easy construction
of a Thomson-Varley precision divider for use in the service shop.
Fig. 1. - Attenuators usually found in test equipment
(A) are not accurate. In another type (B), the pot may load
the divider resistors, upsetting accuracy.
Fig. 2. - This precision divider uses a potentiometer
in the second decade.
Fig. 3 - This decade unit shows how precision dividers
may be cascaded.
For calibrating voltmeters, as an attenuator for signal generators,
to provide accurate gain control, or for voltage comparison and
amplifier measurements, the Thomson-Varley divider is hard to beat.
This decade voltage divider is functional and easy to use. Nevertheless,
many technicians and engineers have never heard of this useful circuit.
Usually, those who know it do not use it because they think special
unavailable switches are necessary.
Contrary to this widespread belief, the Thomson-Varley divider
does not require esoteric switches or circuit arrangements. It can
easily be built around switches available at even the smallest radio
What is a Thomson-Varley divider? To answer this we must look
at attenuators or voltage dividers in general. The type of attenuator
usually found in radio test equipment, such as audio signal generators
and voltage calibrators, is shown in Fig. 1A.
The attenuator switch, in this circuit, is really a range-setting
switch for the output potentiometer labeled Rp Potentiometer
Rp always varies the output from zero to the highest
value permitted by the switch position. This circuit does not allow
precise or accurately known voltage-division ratios. As can be seen,
it is not a decade divider. With a true decade divider, the setting
of any dial does not affect the volts-per-division (or "scale factor,"
as it is called) of any other dial.
Someone may do a little thinking and suggest Fig. 1B as a possible
decade divider. For this circuit, the potentiometer Rp
would shunt across any single divider resistor. The output,
then, is determined by the voltage drops across the switch resistors
and the potentiometer moving contact to ground.
This is not a practical circuit, however, unless the resistance
value of Rp is at least one hundred times larger than
any of the single resistors. Otherwise, the shunt resistance of
Rp would reduce the voltage drop of any switch resistor
that it was connected across. In some applications, Rp
would have to be one thousand times larger than a single switch
resistor in order to reduce the loading to an acceptable value.
True Decade Division
A modification can make this circuit into a true decade divider.
We can do this by making the resistance of Rp exactly
equal to one of the switch resistors. Then, if we have a special
switch that substitutes Rp for any single switch resistor
we wish, we have a true decade divider.
If Rp is inserted in place of R1, for example,
the voltage available at the output can be varied, by Rp,
from zero to one-tenth of the input. Substituting for R2,
Rp varies the output from one-tenth to two-tenths of
the input, and so on. Unfortunately, this system requires a switch
that is just too complicated to be really practical for widespread
use. Nevertheless, various forms of this type of circuit are sometimes
found in special test circuits.
Varley and Thomson - the latter may be more quickly recognized
as Lord Kelvin - were both men of rare mental agility. They evolved
a circuit that provided true decade voltage division, yet overcame
many of the problems involved. However, even their arrangement generally
demands a difficult-to-obtain selector switch. Fortunately, this
final obstacle can be skirted by wiring - and interconnecting a
standard two-gang selector switch. The result is a simple circuit
that is relatively easy to wire.
If each vertical row of contacts in Fig. 2 is considered to be
one of the two wafers or poles in the 10-position switch used, the
desired simplicity of operation can be achieved using the common
type of switch mentioned plus the few relatively inexpensive resistors
and the potentiometer.
Operation of the Divider
Fig. 2 shows this circuit. As with all Thomson-Varley dividers,
there are eleven resistors in the string of switch resistors. The
potentiometer Rp, at any position of the switch, connects
across two of the switch resistors. Of course, the shunting condition
previously noted still exists, but the Thomson-Varley circuit actually
controls this effect and puts it to good use. This is made possible
simply by adding an extra resistor.
Notice, again, that potentiometer Rp connects across
two switch resistors in any position. If we make the value of Rp
exactly equal to the resistance of these two resistors, the total
resistance of the divider is 10R. This is true because a resistance
of 2R in parallel with another resistance of 2R is, of course, equal
to R. Thus a drop of one-tenth of the input voltage is developed
across Rp at all times.
This circuit of Fig. 2 is very useful in the shop and laboratory.
For example, if the dial of potentiometer Rp is divided
into one hundred divisions, we can select any portion of the input
voltage with a resolution of one thousand scale divisions!
To show how easy it is to read this type of divider, suppose
one hundred volts is applied to the input. Now, if the switch is
set to five and the potentiometer dial to fifty-six, the output
is, very simply, 55.6 volts.
For shop use, the resistors may be 1% deposited-carbon or even
selected 5% composition types. Even a seventy-five cent replacement
wirewound control could be used for the potentiometer Rp.
The Thomson-Varley divider, like any other, is never any better
than its components, of course; yet inexpensive components are quite
satisfactory for most shop applications.
Components must be much better for laboratory use. The resistors
must be accurate to 0.1%, or better, and the potentiometer should
be a standard laboratory unit or a multi-turn type. The Helipot
brand is representative.
It is important that a multi-turn potentiometer with zero-resistance
at zero-setting be used, otherwise residual output voltages result.
For this same reason, in high-accuracy laboratory applications,
switches with very low contact resistance must be used, since voltage
drops across such resistances appear in the output.
For shop use, practically any two-gang switch will do. The Centralab
types 1412 and 1413 are suitable. For laboratory applications, laboratory-quality
switches, like those manufactured by Shallcross or Daven, are a
To allow adjustment, it may be advantageous to buy a potentiometer
of somewhat higher resistance than necessary. It can then be shunted
down to exactly the necessary value with parallel resistors.
The circuit in Fig. 2 uses a potentiometer for the "second decade."
Sometimes, it is more desirable to use a tapped resistance in this
second decade. An instrument may be needed that divides the output
into, say, one part in ten thousand. This can be done with four
Not many people will ever wish to build a four-decade divider
- a three-decade unit is a more practical project. Fig. 3 shows
such a three-decade divider, which would require the very best of
components. Although it would be useful only in the laboratory,
it is educationally important since it shows how Thomson-Varley
dividers can be cascaded.
The resistors in each succeeding decade divider must be exactly
one-fifth of the value of those in the preceding decade. This way,
the total resistance of each decade is always equal to the resistance
of two of the resistors in the preceding decade.
The third decade is conventional. But notice that it has eleven
switch positions and ten resistors. Because the third decade has
ten positions, the three decades can be set to 999 and then one
additional step on the last decade adds one to this, bringing the
output to 1000, which is unity. This means the output is equal to
the input and there is no attenuation. The fact that this last switch
has eleven positions is no problem. Eleven-position switches are
common. This last divider arrangement could be used with Fig. 2
in place of the potentiometer. It is simply a matter of replacing
a continuously variable attenuator with a calibrated step attenuator.
The Thomson-Varley decade divider is equally useful for both
d.c. and a.c. applications. Using a value of 1000 ohms for the resistance
of R, the circuit of Fig. 2, when fed with a standard clipped sine
wave, makes an excellent voltage calibrator for the oscilloscope.
Connected to a bank of mercury cells, the decade divider is excellent
for calibrating voltmeters and the like. Since the meter produces
a loading error, the value of R should be lower. One hundred ohms
would be an approximate total decade resistance for this application.
The value of R would then be ten ohms.
Test instruments and signal generators need accurate decade attenuators
and gain controls. This responsibility is easily taken care of by
a Thomson-Varley divider.
Amplifier gain can be very accurately measured, at all frequencies,
with the Thomson-Varley circuit. It is thus useful for running either
frequency-response curves or making absolute voltage-gain measurements.
To check gain, connect a Thomson-Varley divider to the output of
an amplifier or amplifier stage. Then use a single-pole, double-throw
switch to connect the vertical-deflection terminals of an oscilloscope
to either the amplifier input or the divider output.
Now adjust the divider until its output, as shown on the scope,
is equal to the amplifier input. The amount of attenuation required
from the divider to exactly counterbalance the amplifier gain, which
can be read easily from the markings on the divider, gives an accurate
picture of the amplifier's gain. Suppose that the divider at the
output of an amplifier stage must be adjusted to one-tenth the voltage
across the entire combination in order to match the input voltage
measured at the grid of' this same stage. This would mean that the
stage has a gain of 10.
An advantage of this method of gain measurement is that it is
not affected by irregularities in the response of the oscilloscope,
meter, or other device used to take the measurement, by variation
in oscillator output, or by the many other concealed factors that
may introduce errors into the measurement procedure.
The applications noted here are by no means a complete listing.
Once the technician has taken the trouble to build such a divider,
he will continue to find additional uses for it. If desired, the
circuit of Fig. 2 can be built into a small aluminum case for bench
use. The cost should be only a few dollars if deposited-carbon resistors
Posted October 2, 2014