Mechanical Meter Movements
September 1960 Popular Electronics
meter movements have been around since the late 1800s. In 1882 Jacques-Arsène d'Arsonval and Marcel Deprez developed
a meter movement with a stationary permanent magnet and a moving coil of wire which survives today as the dominant
form. Lord Kelvin's galvanometer preceded d'Arsonval's by a decade or so, but it relied on the Earth's magnetic field
and needed to be properly oriented to work. d'Arsonval's movement incorporated a permanent magnet instead to improve
sensitivity and convenience. I'm not sure d'Arsonval gets sole billing on the name - why not the Deprez movement?
This article in Popular Electronics from 1960 is as relevant today as it was half a century ago.
September 1960 Popular Electronics
of Contents]People old and young enjoy waxing nostalgic about and learning some of the history of early electronics.
Popular Electronics was published from October 1954 through April 1985. All copyrights (if any) are hereby acknowledged.
MetersBy Ken Gilmore
great English scientist, Lord Kelvin, once said, "When you can measure what you are speaking about and express it
in numbers, you know something about it." Following Lord Kelvin's line of thought, if we are to know something about
electricity and electronic instruments, we must have rugged, convenient, accurate instruments able to measure a wide
variety of voltages, currents, and resistances. The "meter" is such an instrument.
This most basic of all test
instruments has actually not undergone a single change in fundamental theory or design since 1888. It was in that
year - almost 20 years before the invention of the triode vacuum tube - that Edward Weston developed the device we
now know as the Weston movement.
The Weston Movement.
Figure 1(A) shows a single coil
of wire suspended between the north and south poles of a magnet. Figure 1(B) is a cross section of this setup; the
arrows indicate the direction of the magnetic lines of force. When current begins to flow in the wire, a magnetic
field forms around it as shown by the small circles. This field opposes the field of the permanent magnet so that
the coil is forced to rotate as shown. Since the force generated by one turn is very weak, many turns are used in
Figure 2 shows such a coil with a needle attached to it; the needle moves along a calibrated
scale as the coil rotates. The distance the needle moves is proportional to the amount of current flowing. In other
words, if 0.5 ma. generates a magnetic field powerful enough to deflect the needle to half scale, then 1 ma. will
cause full-scale deflection. Figure 3 shows the actual construction of a Weston movement - the moving coil (A), a
magnet and core (B), and the complete movement (C).
Only one aspect of the Weston movement has changed with succeeding years. (See Fig. 4). Development of better magnetic
steels has allowed designers to make a more compact instrument by putting the magnet inside the moving coil; the iron
shell around the coil completes the magnetic path.
Mechanical meter movements
Mechanical meter movement diagram.
Mechanical meter movement magnet.
Mechanical meter movement coil.
Mechanical meter movement diode bridge for AC input.
Typical multimeter with mechanical movement.
Mechanical meter movement range selection schematic.
Schematic for meter movement
Measuring external resistance.
Bear in mind that the Weston movement is a d.c. instrument.
If a.c. is applied, the needle will try to follow each reversal of the current. But since it cannot move fast enough,
it remains in one place and vibrates. But the Weston movement can measure a.c. currents with the addition of a simple
rectifier. Figure 5 shows the basic full-wave circuit commonly used.
This ability of a Weston movement to respond
to either a.c. or d.c. current - with the proper circuitry - makes possible one of the most useful test instruments
in electronics: the multimeter. (See Fig. 6.) By adding a handful of resistors, rectifiers, and switches to the meter
movement, we come up with a versatile instrument that can measure not only a.c. and d.c. current, but also voltage
Let's suppose we have a meter with a basic 1-ma.
movement. This means that if 1 ma. of current flows through the coil, the needle will be deflected to its full-scale
reading. But say we want to measure a current of 2 ma. We can do it by using a "shunt." To our British friends, this
word means a railroad siding. In electronics, it also means a siding, but one for electrons rather than trains. In
Fig. 7, the resistance of shunt RS1 is equal to the resistance of the meter (Rm). Thus, half
the current (Im) will flow through the meter, the other half (Is) through the shunt, and the
full-scale deflection of the needle represents 2 ma.
Shunts are easily calculated if we know the meter's internal
resistance (Rm). In this case, let's say Rm = 100 ohms. Thus, RS1 in the example
given would also be 100 ohms. If the shunt were 50 ohms (RS2), twice as much current would flow through
the shunt as through the meter. The meter would conduct only one-third the total current, and its full scale deflection
would represent 3 ma. If the shunt were approximately 11 ohms (RS3), nine times as much current would flow
through the shunt as through the meter, or, conversely, one tenth the total would flow through the meter, and the
full-scale sensitivity would be 10 ma.
Modern multimeters have a number of different shunts which can be switched
into the circuit to give different current ranges. One typical meter on the market, for example, has scales of 1.5
ma., 15 ma., 150 ma., 500 ma., and 15 amperes. Incidentally, the shunting circuits work the same way in both a.c.
and d.c. circuits; the only difference is that a rectifier must be in the circuit for the meter to read a.c.
So far, we have considered only current measurements. But a meter
can be connected to measure voltage as well. Let's take that same basic 1-ma., 100-ohm meter movement again and make
a voltmeter out of it. By using Ohm's law, we can find the voltage which must be applied across the meter terminals
to make a 1-ma. flow: E = IR; E = .001 x 100; E = .1 volt.
If more than .1 volt appears across the terminals,
more than 1 ma. will flow through the meter and damage or destroy it. But suppose we want to measure 100 volts. Again,
we apply Ohm's law to find out what resistance the meter would need for only 1 ma. to flow if 100 volts were applied:
R = E/I; R = 100/.001; R = 100,000 ohms.
Since the basic movement is only 100 ohms, we simply add the 99,900
ohms to make up the total of 100,000 in series with the movement as shown in Fig. 8. With various resistances switched
into the circuit, one meter can measure a wide range of voltages. One typical commercial meter, for example, has ranges
of 1.5 volts, 5 volts, 150 volts, 500 volts, 1500 volts, and 5000 volts. Again, both a.c. and d.c. voltage ranges
can be measured by switching in the rectifier for alternating current.
A basic meter movement can even be made to measure resistance, but this requires an additional circuit
component - a battery. Let's take our 1-ma., 100-ohm meter movement and connect a 50-volt battery in series with one
of the leads, as shown in Fig. 9. Again, Ohm's law comes into the picture. We know we have 50 volts in the circuit,
and the meter movement must not conduct more than 1 ma., so we can calculate the minimum resistance that must be included
in the circuit to limit the current to a 1-ma. value: R=E/I; R=50/.001; R=50,000 ohms.
Since the meter already
has an internal resistance of 100 ohms, we need add only the other 49,900 in series (R1). Now if we short
the two test leads together, 1 ma. of current will flow and the meter will read full scale. Any additional resistance
introduced into the circuit will cause the meter to read somewhere between full scale and zero. A relatively low resistance
(Rx) between the test leads, for example, would perhaps make the meter read nine-tenths full scale; a larger
resistance would make it read half scale; with an infinite resistance, no current at all would flow.
we see that zero ohms appears on the right end of the scale, or opposite from the zero of the volt and ampere scales.
Because of the inherent characteristics of the ohmmeter, the needle becomes more and more inaccurate as it approaches
the left side of the scale. Therefore, technicians usually try to take resistance readings as near the center of the
scale as possible, to obtain the most accurate readings. They do this by switching to various ranges, which, in turn,
means switching batteries of different voltages into the circuit. In practice, also, a small variable resistor is
usually included in the ohmmeter circuit to compensate for variations in battery strength. The knob controlling this
resistor is usually labeled "Ohms Adjust" on the front panel of the multimeter.
Meter movement product applications.
The basic Weston movement can be incorporated into still other kinds of circuits containing vacuum tubes.
These instruments have certain advantages over the conventional multimeter just described, and are particularly useful
for some types of work. (See Test Instruments: The Vacuum-Tube Voltmeter; April, May, July, 1959, P.E.)
for certain kinds of vacuum-tube voltmeters, all multimeters have one great shortcoming: they can measure a.c. voltages
at relatively low frequencies only - up to about 20,000 cps. But radio and television stations and other branches
of communications must measure r.f. voltages and currents up to hundreds of megacycles. This is done with the help
of the thermoelement - two tiny chunks of metal, frequently constantan and platinum, clamped together. When the metals
are heated, they generate a small voltage across the junction between them. Thus, a circuit can be designed so that
r.f. voltage flowing through a separate conductor will heat the junction, which then generates a voltage proportional
to the amount of heating. This current is measured by a Weston movement, calibrated in terms of r.f. current.
Designers, using the Weston movement as the basic indicator, have come up with an astonishing bag of tricks over
the years. With the addition of a light-sensitive selenium disc, for example, as shown in Fig. 10, the device becomes
a commercial photographic exposure meter - the brighter the light on the disc, the more current generated. A small
generator, on the other hand, transforms the meter into a tachometer for measuring rpm. In another application, two
meters in one case can be connected to the electronic receivers in an aircraft instrument landing system and arranged
so that they show the pilot whether he is on or off course (Fig. 11). Such meter applications are virtually endless.
Although the basic Weston movement has not changed in principle or
basic design for 72 years, there are many striking new developments in meters. One of the newest is a printed-circuit
meter recently introduced by the Parker Instrument Division of Interlab, Inc. As shown Fig. 12 the meter's coil is
printed on a thin disc and mounted parallel to a ring magnet. When current flows through the printed-circuit coil,
a magnetic field is created which reacts with the field of the magnet, and makes the disc rotate. A soft iron shell
(not shown) encloses the magnet and disc, furnishing a return path for the magnetic lines of force.
Printed circuit meter movement.
The entire printed-circuit meter is only 1/2-inch thick. And since it weighs only a fraction as much as conventional
meters of similar sensitivity and range, it will undoubtedly find widespread use where size and weight are important
- in airborne equipment, for example. Another important advantage of the new movement is its ability to handle overloads
that would instantly burn out the relatively delicate Weston movement. The manufacturer claims that an overload of
1000 to 5000% will not damage these movements.
Another relatively new development is the meter which triggers
a relay. Here, the indicating needle is fitted with a contact. A matching contact is fastened to an arm which is adjustable
from the front panel. When the current in the circuit under measurement causes the needle to deflect to where the
adjustable arm has been pre-set, the two contacts come together and set off a sensitive relay which can then be used
to control some other circuit. By far the most sensitive relays available, these instruments can be made to operate
on as little as one or two microamperes. Units of this type, by the way, can be used in any kind of control circuit-
battery charging, tube overload protection, etc. - anywhere fast, accurate control is needed.
such as these only scratch the surface. As the science of electronics advances into new realms, scientists and engineers
are constantly finding new ways to make the basic meter - oldest of all electronic test instruments - more and more