Module 21—Test Methods and Practices
Pages i - ix
1-1 to 1-10
, 1-11 to 1-20
1-21 to 1-26
, 2-1 to 2-10
2-11 to 2-20
, 2-21 to 2-30
2-31 to 2-40
, 2-41 to 2-48
3-1 to 3-10
3-11 to 3-20
, 3-21 to 3-30
3-31 to 3-39
, 4-1 to 4-10
4-11 to 4-14
, 5-1 to 5-10
5-11 to 5-20
5-21 to 5-30
, 5-31 to 5-35
to AI-3, Index
Exercise caution in using a stroboscope. The illusion of stopped motion is very convincing. Do
not attempt to touch the moving equipment.
Q-19. If you are required to monitor the speed of a
device with a stroboscope over an extended period of time, what step should be taken to prolong the life of the
Frequency Counter Methods
Various frequency counters have found
application as an ELECTRONIC TACHOMETER to obtain accurate measurements of high-speed rotating machinery. A
tachometer pickup may be used to produce signals that are fed directly to the frequency counter. If the tachometer
pickup is designed to generate 1 signal per revolution, the counter will indicate directly in revolutions per
second; if the pickup is designed to produce 60 signals per revolution, the counter will indicate directly in
revolutions per minute.
Audio-frequencies can be measured
with a variety of nonelectronic and electronic devices. Examples of nonelectronic measuring devices are the
vibrating-reed meter and the moving-disk frequency meter. (Both of these devices were discussed in NEETS, module
3.) They are used primarily to measure the frequency of ac power, 60 Hz. However, such instruments do not have a
wide frequency range. The most common instruments available for the measurement of audio frequencies are
oscilloscopes and frequency counters.
The frequency of a waveform can readily be determined by using an
oscilloscope. The most common oscilloscope method of measuring a frequency is accomplished by first measuring the
time duration of the waveform. Frequency is the reciprocal of time
and may be easily computed, as shown in figure 3-24.
Figure 3-24.—Oscilloscope method of determining frequency.
Another common method of determining the frequency of a waveform is by using Lissajous patterns. This
method was discussed in NEETS, module 19.
FREQUENCY COUNTER METHOD
oscilloscopes can be used to compare rectangular waveforms for the purpose of measuring the frequency of a signal,
frequency counters, as shown in figure 3-25, are much more useful for this purpose. The fundamental measurement of
frequency is accomplished by totaling the number of cycles into the counter for a precise period of time. The
result is then displayed as an exact digital readout. The audio- frequency signal must be of sufficient amplitude
to trigger the counter. The AUTO-MANUAL switch provides two methods of frequency counter operation. One method is
to initiate the count simultaneously with the initiation of the signal to be measured. With this method, the
AUTO-MANUAL switch should be set to the MANUAL position. The second method assumes that the signal to be measured
has been operating over some indefinite period of time and that it will continue to do so after a measurement has
been taken (hence, only that segment of the signal required to make the frequency measurement is important). With
this method, the AUTO-MANUAL switch is to be set to the AUTO position.
Figure 3-25.—Frequency counter.
RADIO-FREQUENCY (RF) MEASUREMENTS
Radio-frequency measurements are primarily
made with frequency counters. Most oscilloscopes are limited in use to approximately 100 MHz. Frequency meters,
such as the Hewlett-Packard 530 series, are widely used but lack the accuracy of frequency counters.
Prior to the invention of the frequency counter, most frequency
measurements above the af range were made primarily with frequency meters.
This process involved
heterodyning the frequency to be measured against the calibrated output of the frequency meter to obtain a zero
beat from which the measured frequency was then read. This method proved inaccurate because of reading errors.
Frequency meters as we know them today are entirely different from their predecessors. Today's frequency
meters (fig. 3-26) contain waveguide or coaxial lines coupled to quarter-wavelength resonant cavities. The meter
is adjusted until the cavity is tuned to the resonant frequency of the signal being measured. At resonance, power
is absorbed by the cavity and produces a dip in the output-power level, as measured at the frequency meter's
output connector. The resonant frequency is read directly from the frequency meter dial and is accurate, in most
cases, to approximately ±0.2%. Frequency meters are capable of measuring frequencies in the range of 1 to 40
gigahertz, far exceeding the frequency limitations of the average frequency counter.
Q-20. What happens
when a frequency meter is adjusted to the frequency of the signal being measured?
Figure 3-26.—Frequency counter.
In the early 1950s, the frequency counter was developed. The
device could measure and accurately indicate frequencies up to 10 MHz. Present-day frequency counters can
accurately read frequencies as high as 40 GHz. In addition to direct frequency measurement indication, some types
of frequency counters can measure the WAVE PERIOD, which is the inverse of frequency; RATIO, which compares one
frequency against another; and TIME INTERVAL, the time between two events or the time between two functions of an
event. In addition, frequency counters can totalize event indications. This is similar to measuring the frequency
except that a manual or an electronic start-stop gate controls the time over which the measurement is taken.
Frequency counters can also provide scaling in the form of a digital output signal from the frequency counter that
represents a frequency-related division of the input frequency.
All of the above functions have useful
applications. For pulse timing, the period function is used; totalizing is used in digital applications; and ratio
is used in comparing harmonic-related signals. Scaling is used for triggering other test equipment used in
conjunction with the frequency counter; and time- interval capability is used in measuring the interval between
two pulses or between two sets of pulses. Because of the wide variety of frequency counters in use, the technical
manual for a specific frequency counter should be consulted to determine the instrument's full capabilities.
Frequency Counter Accuracy
All frequency counter measurements are measured with 1 part in 108 of accuracy. However, frequency counters have
provisions for input from external frequency standards. This extends the accuracy of the frequency to that of the
standard. A frequency self-check capability is provided to determine if the counting and lighting circuits are
Wavemeters are calibrated resonant circuits used to measure
frequency. Although the accuracy of wavemeters is not as high as that of heterodyne frequency meters, they have
the advantage of being comparatively simple and can be easily carried about.
Any type of resonant circuit
may be used in wavemeter applications. The exact kind of circuit employed depends on the frequency range for which
the meter is intended. Resonant circuits consisting of coils and capacitors are used for low-frequency wavemeters.
Butterfly circuits, adjustable transmission line sections, and resonant cavities are used in vhf and microwave
There are three basic kinds of wavemeters: the absorption, the reaction, and the transmission types. Absorption
wavemeters are composed of the basic resonant circuit, a rectifier, and a meter for indicating the amount of
current induced into the wavemeter. In use, this type of wavemeter is loosely coupled to the circuit to be
measured. The resonant circuit of the wavemeter is then adjusted until the current meter shows a maximum
deflection. The frequency of the circuit under test is then determined from the calibrated dial of the wavemeter.
The reaction type derives its name from the fact that it is adjusted until a marked reaction occurs in the
circuit being measured. For example, the wavemeter is loosely coupled to an oscillator, and the resonant circuit
of the meter is adjusted until it is in resonance with the oscillator frequency. The setting of the wavemeter dial
is made by observing the output current of the oscillator. At resonance, the wavemeter circuit takes energy from
the oscillator, causing the current to dip sharply. The frequency of the oscillator is then determined from the
calibrated dial of the wavemeter.
The transmission wavemeter is an adjustable coupling link. When it is inserted between a source of rf energy and
an indicator, energy is transmitted to the indicator only when the wavemeter is tuned to the frequency of the
source. Transmission wavemeters are widely used in measuring microwave frequencies.
In figure 3-27, a
typical cavity wavemeter is illustrated.
Figure 3-27.—Typical cavity wavemeter.
The wavemeter illustrated is of the type commonly used for the measurement of microwave frequencies. The
device employs a resonant cavity, which effectively acts as a high-Q LC tank circuit. The resonant frequency of
the cavity is varied by means of a plunger that is mechanically connected to a micrometer mechanism. Movement of
the plunger into the cavity reduces the cavity size and increases the resonant frequency. Conversely, an increase
in the size of the cavity (made by withdrawing the plunger) lowers the resonant frequency. The microwave energy
from the equipment under test is fed into the wavemeter through one of two inputs, A or D. A crystal rectifier
then detects or rectifies the signal, and the rectified current is indicated on the current meter, M.
instrument can be used as either a transmission type or an absorption type of wavemeter. When used as a
transmission wavemeter, the unknown signal is coupled into the circuit by means of input A. When the cavity is
tuned to the resonant frequency of the signal, energy is coupled through coupling loop B into the cavity and out
through loop C to the crystal rectifier where it is rectified and indicated on the meter. At frequencies off
resonance little or no current flows in the detector and the meter reading is small. Therefore, the micrometer and
attached plunger are varied until a maximum meter reading is obtained. The micrometer setting is then compared
with a calibration chart supplied with the wavemeter to determine the unknown frequency.
When the unknown
signal is relatively weak, such as the signal from a klystron oscillator, the wavemeter is usually used as an
absorption type of device. Connection is made to the instrument at input D. Rf loop C then acts as an injection
loop to the cavity. When the cavity is tuned to the resonant frequency of the klystron, maximum energy is absorbed
by the cavity, and the current indicated on the meter dips. When the cavity is not tuned to the frequency of the
klystron, high current is indicated on the current meter. Therefore, the cavity is tuned for a minimum reading, or
dip, in the meter; and the resonant frequency is determined from the micrometer setting and the calibration chart.
The potentiometer, R1, is used to adjust the sensitivity of the meter from the front panel of the
instrument. J1 is a video jack and is provided for observing video waveforms with a test oscilloscope.
The following is a brief summary of the important points of this chapter.
IMPEDANCE BRIDGES have several things in common. Each type of bridge has a comparing circuit and a
measuring circuit. They measure an unknown impedance by comparing the characteristics of the device under test
with the characteristics of components within the test set.
POWER METERS that are
designed to measure af power can be separated into two distinct groups. Power meters that are designed for
measuring sine waves are basically electronic voltmeters calibrated in dB or dBm. VU METERS are designed to
measure the average value of complex waveforms, such as a voice.
The most common type of test equipment used to measure rf power is the ABSORPTION POWER METER.
Absorption power meters are designed to absorb all or part of the signal being measured. Examples of absorption
power meters are output power meters, in-line wattmeters, and meters employing bolometers.
CALORIMETERS are the most accurate type of test equipment used for measuring high
power. As power is applied to a calorimeter, its medium (either liquid or solid) is heated. The heat that is
produced is directly proportional to the amount of applied power. The amount of applied power is determined by
measuring the change in temperature of the medium.
Today's ELECTRONIC FREQUENCY COUNTERS
are capable of measuring frequencies from dc to 40 GHz. Most have added features that enable period averaging,
time-interval measurements, and scaling. Frequency counter accuracy can be extended by using an external frequency
standard in lieu of its internal frequency standard.
Coaxial Frequency Meter, NAVSHIPS 0969-092-3010, Naval Ships Systems Command, Washington, D.C., 1978.
EIMB, Test Methods and Practices, NAVSEA 08967-LP-000-0130, Naval Sea Systems Command, Washington, D.C., 1980.
Fire Control Technician (M) 3 & 2, NAVEDTRA 10209-A, Naval Education Training and Program Development Center,
Pensacola, Fla., 1974.
NEETS, Module 16, Introduction to Test Equipment, NAVEDTRA 172-16-00-84, Naval Education and Training
Professional Development and Technology Center, Pensacola, Fla., 1984.
ANSWERS TO QUESTIONS Q1 THROUGH Q20.
A-1. A bridge circuit is balanced when the opposite legs of the comparing and measuring circuits
exhibit the same voltage drop.
A-2. The capacitive and inductive characteristics of the test leads.
A-3. As the supply voltage increases, bridge components may heat up and become less accurate.
A-4. Small values of resistances.
A-5. A standard capacitor.
A-6. Both measure phase angle and magnitude in determining impedance.
A-7. High VSWR, which equates to poor reception or a loss of power output.
A-8. DB, dBm, and
A-9. 600-ohm load.
A-10. dB meters are used for measuring sine waves. Vu meters are
used to measure the average value of complex waveforms.
A-11. Current transformers.
A-12. Electronic wattmeters are capable of measuring high-frequency signals.
A-13. Most in-line
wattmeters are capable of measuring both forward and reflected power.
material that exhibits a large negative temperature coefficient.
A-15. Temperature, mass, and time.
A-16. As power is applied, the medium heats up in proportion to the applied power.
National Bureau of Standards.
A-18. They are used to monitor fixed motor speeds.
Monitor a submultiple frequency to prolong the flasher-tube life.
A-20. Power is absorbed by the
frequency meter cavity; and a pronounced dip in power, at the output, will be observed.
Introduction to Matter, Energy, and Direct Current,
to Alternating Current and Transformers, Introduction to Circuit Protection,
Control, and Measurement
, Introduction to Electrical Conductors, Wiring Techniques,
and Schematic Reading
, Introduction to Generators and Motors
Introduction to Electronic Emission, Tubes, and Power Supplies,
Introduction to Solid-State Devices and Power Supplies
Introduction to Amplifiers, Introduction to
Wave-Generation and Wave-Shaping Circuits
, Introduction to Wave Propagation, Transmission
Lines, and Antennas
, Microwave Principles,
, Introduction to Number Systems and Logic Circuits, Introduction
to Microelectronics, Principles of Synchros, Servos, and Gyros
Introduction to Test Equipment
, Radar Principles,
The Technician's Handbook,
Master Glossary, Test Methods and Practices,
Introduction to Digital Computers,
Magnetic Recording, Introduction to Fiber Optics