Navy Electricity and Electronics Training Series (NEETS), Module 16

Module 16 − Introduction to Test Equipment

Pages i, 1−1, 1−11, 1−21, 2−1, 2−11, 2−21, 3−1, 3−11, 3−21, 3−31, 4−1, 4−11, 4−21, 5−1, 5−11, 5−21, 5−31, 6−1, 6−11, 6−21, 6−31, 6−41, Index

The normal speed range is from 110 to 25,000 rpm. At speeds below 600 rpm, "flicker" becomes a problem because the human eye cannot retain successive images long enough to create the illusion of continuous motion. The life of the strobotron lamp is approximately 250 hours if used at flashing speeds of less than 5,000 rpm, or 100 hours if used at higher speeds.

All alternating voltage sources are generated at a set frequency or range of frequencies. A Frequency METER provides a means of measuring this frequency. The electrical output frequency of ac power generators can be measured by a vibrating reed, a tuned circuit, or by a crossed-coil, iron-vane type meter. The vibrating-reed device is the simplest type of frequency meter. It has the advantage of being rugged enough to be mounted on generator control panels.

A simplified diagram of a vibrating-reed frequency meter is shown in figure 2-8, views a through D. In view A, you can see that the current to be measured flows through the coil and exerts maximum attraction on the soft-iron armature twice during each cycle. The armature is attached to the bar, which is mounted on a flexible support. Reeds of suitable dimensions to have natural vibration frequencies of 110, 112, 114, and so forth, up to 130 hertz are mounted on the bar (view B). The reed with a frequency of 110 hertz is marked 55 hertz; the one with a frequency of 112 hertz is marked 56 hertz; the one with a frequency of 120 hertz is marked 60 hertz, and so forth.

When the coil is energized by a current with a frequency between 55 and 65 hertz, all the reeds are vibrated slightly; but, the reed having a natural frequency closest to that of the energizing current vibrates through a larger amplitude. The frequency is read from the scale value opposite the reed having the greatest amplitude of vibration.

In some instruments, the reeds are the same length; but they are weighted by different amounts at the top so they will have different natural rates of vibration. An end view of the reeds in the indicator is shown in view C. If the energizing current has a frequency of 60 hertz, the reed marked 60 will vibrate the

greatest amount, as shown. View D shows a hand-held vibrating-reed frequency meter mounted on the casing of a motor-generator.

Tuned Circuits are used as filters for the passage or rejection of specific frequencies. Bandpass FILTERS and Band-REJECT FILTERS are examples of this type. Tuned circuits have certain characteristics that make them ideal for certain types of filters, especially where a high degree of selectivity is desired. a series-tuned circuit offers a low impedance to currents of the particular frequency to which the circuit is tuned and a relatively high impedance to currents of all other frequencies. a parallel-tuned circuit, on the other hand, offers a very high impedance to currents of its natural, or resonant, frequency and a relatively low impedance to others. If you feel you need to review the subject of tuned circuits at this time, refer to NEETS, Module 9, Introduction to Wave-Generation and Wave- Shaping Circuits, for more information on these circuits and their applications.

Frequency measurements in the AF range can be made by the comparison method or the direct- reading frequency meter. Frequency comparisons can be made by the use of a calibrated af generator in conjunction with either an oscilloscope or a modulator and a zero-beat indicating device. Direct-reading frequency measurements can be made by instruments using series, frequency-selective electrical networks, bridge test sets having null indicators, or counting-type frequency meters.

Heterodyne frequency meters are available in several varieties. They measure the frequency of the unknown signal by matching the unknown signal with a locally generated signal of the same frequency obtained from a calibrated, precision oscillator. This method is normally referred to as zero beating. When a perfect frequency match is obtained, it is indicated by the absence of a beat note (zero beat). The technician generally uses a set of headphones to detect a zero-beat condition in the equipment being tested.

The basic heterodyne meter (figure 2-9) is a calibrated variable oscillator, which heterodynes against the frequency to be measured. Coupling is accomplished between the frequency meter and the output of the equipment under test. (Note: This coupling should be in accordance with the step-by-step procedures listed in the technical manual for the frequency meter.) The calibrated oscillator is then tuned so that the difference between the oscillator frequency and the unknown frequency is in the af range. This difference in frequency is known as the BEAT Frequency. As the two frequencies are brought closer to the same value, the tone in the headset will decrease in pitch until it is replaced by a series of rapid clicks. As the process is continued, the clicks will decrease in rapidity until they stop altogether. This is the point of zero beat; that is, the point at which the frequency generated in the oscillator of the frequency meter is equal to the frequency of the unknown signal being measured.

Q-7. In a heterodyne-type frequency meter, what is the difference between the oscillator frequency and the unknown frequency?

For all practical purposes, the point of zero beat can be assumed when the clicks are heard at infrequent intervals. Figure 2-10 illustrates the zero-beat concept. Maintaining a condition of absolute silence in the earphones is extremely difficult when you are making this measurement. When the incoming signal is strong, the clicks are sharp and distinct. When the signal is weak, the zero-beat condition is evidenced by a slowly changing "swishing" or "rushing" sound in the headset. After the zero beat is obtained, the dial reading corresponds to the frequency measured.

The manufacturer's calibration book is a very important part of the frequency meter package; in fact, the book is so important that it bears the same serial number as the heterodyne-type frequency meter itself. Contained in this book is a list of the dial settings and the corresponding frequencies produced by that meter at those dial settings. Operating instructions for the meter are also included.

WAVEMETERS are calibrated resonant circuits used to measure frequency. The accuracy of wavemeters is not as high as that of heterodyne-type frequency meters; however, they have the advantage of being comparatively simple and can be easily carried.

Any type of resonant circuit can be used in wavemeter applications. The exact kind of circuit used depends on the frequency range for which the meter is intended. Resonant circuits consisting of coils and capacitors are used for VLF through VHF wavemeters.

The simplified illustration of an absorption wavemeter, shown in figure 2-11, consists of a pickup coil, a fixed capacitor, a lamp, a variable capacitor, and a calibrated dial. When the wavemeter's components are at resonance, maximum current flows in the loop, illuminating the lamp to maximum brilliance. The calibrated dial setting is converted to a frequency by means of a chart, or graph, in the instruction manual. If the lamp glows very brightly, the wavemeter should be coupled more loosely to the circuit. For greatest accuracy, the wavemeter should be coupled so that its indicator lamp provides only a faint glow when tuned to the resonant frequency.

The signal frequencies of radio and radar equipments that operate in the UHF and SHF ranges can be measured by resonant, cavity-type wavemeters or resonant, coaxial-line-type wavemeters. When properly calibrated, resonant-cavity and resonant-coaxial line wavemeters are more accurate and have better stability than wavemeters used for measurements in the LF to VHF ranges. These frequency-measuring instruments are often furnished as part of the equipment. They are also available as general-purpose test sets.

Although many wavemeters are used in performing various functions, the cavity-type wavemeter is the type most commonly used. Only this type is discussed in some detail.

Figure 2-12 shows a typical CAVITY WAVEMETER. The wavemeter is of the type commonly used for the measurement of microwave frequencies. The device uses a resonant cavity. The resonant frequency of the cavity is varied by means of a plunger, which 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 being tested is fed into the wavemeter through one of two inputs, A or B. The crystal rectifier then detects (rectifies) the signal. The rectified current is indicated on current meter M.

Another device used to measure frequencies above the audio range is the ELECTRONIC Frequency COUNTER. Since this instrument will be covered in detail in a later chapter, only a brief description is provided at this time.

The electronic frequency counter is a high-speed electronic counter with an accurate, crystal- controlled time base. This combination provides a frequency counter that automatically counts and displays the number of events occurring in a precise time interval. The frequency counter itself does not generate any signal; it merely counts the recurring pulses fed to it.

WAVEforM ANALYSIs can be made by observing displays of voltage and current variations with respect to time or by harmonic analysis of complex signals. Waveform displays are particularly valuable for adjusting and testing pulse-generating, pulse-forming, and pulse-amplifying circuits. The waveform visual display is also useful for determining signal distortion, phase shift, modulation factor, frequency, and peak-to-peak voltage.

Waveform analysis is used in various electrical and electronic equipment troubleshooting. This section will briefly discuss the oscilloscope and spectrum analyzer to provide you with basic knowledge of this test equipment.

The CATHODE-RAY OSCILLOSCOPE (CRO or O-SCOPE) is commonly used for the analysis of waveforms generated by electronic equipment. Several types of cathode-ray oscilloscopes are available for making waveform analysis. The oscilloscope required for a particular test is determined by characteristics such as input-frequency response, input impedance, sensitivity, sweep rate, and the methods of sweep control. The SYNCHROSCOPE is an adaptation of the cathode-ray oscilloscope. It features a wide-band amplifier, triggered sweep, and retrace blanking circuits. These circuits are desirable for the analysis of pulse waveforms.

Oscilloscopes are also part of some harmonic analysis test equipments that display harmonic energy levels. To effectively analyze waveform displays, you must know the correct wave shape. The maintenance instructions manual for each piece of equipment illustrates what waveforms you should observe at the various test points throughout the equipment. Waveforms that will be observed at any one selected test point will differ; each waveform will depend on whether the operation of the equipment is normal or abnormal.

The display observed on a cathode-ray oscilloscope is ordinarily one similar to those shown in figure 2-13. Views a and B show the instantaneous voltage of the wave plotted against time. Elapsed time (view A) is indicated by horizontal distance, from left to right, across the etched grid (graticule) placed over the face of the tube. The amplitude (view B) of the wave is measured vertically on the graph.

The oscilloscope is also used to picture changes in quantities other than simply the voltages in electric circuits. For example, if you need to see the changes in waveform of an electric current, you must first send the current through a small resistor. You can then use the oscilloscope to view the voltage wave across the resistor. Other quantities, such as temperatures, pressures, speeds, and accelerations, can be translated into voltages by means of suitable transducers and then viewed on the oscilloscope. a detailed discussion of the oscilloscope is presented in chapter 6 of this module.

The SPECTRUM ANALYZER is a device that sweeps over a band of frequencies to determine (1) what frequencies are being produced by a specific circuit under test and (2) the amplitude of each frequency component. To accomplish this, the spectrum analyzer first presents a pattern on a display. Then the relative amplitudes of the various frequencies of the spectrum of the pattern are plotted (see figure 2-14). On the vertical, or Y axis, the amplitudes are plotted; on the horizontal, or X axis, the frequencies (time base) are plotted. The overall pattern of this display indicates the proportion of power present at the various frequencies within the SPECTRUM (fundamental frequency with sideband frequencies).

Q-10. What device sweeps a band of frequencies to determine frequencies and amplitudes of each frequency component?

The spectrum analyzer is used to examine the frequency spectrum of radar transmissions, local oscillators, test sets, and other equipment operating within its frequency range. Proper interpretation of the displayed frequency spectrum enables you to determine the degree of efficiency of the equipment under test. With experience, you will be able to determine definite areas of malfunctioning components within equipment. In any event, successful spectrum analysis depends on the proper operation of a spectrum analyzer and your ability to correctly interpret the displayed frequencies. Later, in chapter 6, we will discuss the various controls, indicators, and connectors contained on the spectrum analyzer.

Because of the reliability of semiconductor devices, servicing techniques developed for transistorized equipment differ from those normally used for electron-tube circuits. Electron tubes are usually considered to be the circuit component most susceptible to failure and are normally the first components to be tested. Transistors, however, are capable of operating in excess of 30,000 hours at maximum rating without failure. They are often soldered in the circuit in much the same manner as resistors and capacitors. Therefore, they are NOT so quickly removed for testing as tubes.

Substitution of a semiconductor diode or transistor known to be in good condition is one method of determining the quality of a questionable semiconductor device. This method should be used only after you have made voltage and resistance measurements. This ensures the circuit has no defect that might

damage the substitute semiconductor device. If more than one defective semiconductor is present in the equipment section where trouble has been localized, the semiconductor replacement method becomes cumbersome. Several semiconductors may have to be replaced before the trouble is corrected. To determine which stage(s) failed and which semiconductors are not defective, you must test all the removed semiconductors. You can do this by observing whether the equipment operates correctly as you reinsert each of the removed semiconductor devices into the equipment.

Semiconductor diodes, such as general-purpose germanium and silicon diodes, power silicon diodes, and microwave silicon diodes, can be tested effectively under actual operating conditions. However, crystal-rectifier testers are available to determine dc characteristics that provide an indication of crystal- diode quality.

A common type of crystal-diode test set is a combination ohmmeter-ammeter. Measurements of forward resistance, back resistance, and reverse current can be made with this equipment. Using the results of these measurements, you can determine the relative condition of these components by comparing their measured values with typical values obtained from test information furnished with the test set or from the manufacturer's data sheets. a check that provides a rough indication of the rectifying property of a diode is the comparison of the back-and-forward resistance of the diode at a specified voltage. a typical back-to-forward-resistance ratio is on the order of 10 to 1, and a forward-resistance value of 50 to 80 ohms is common.

Q-11. What is the typical back-to-forward resistance ratio of a good-quality diode?

A convenient test for a semiconductor diode requires only an ohmmeter. The back-and-forward resistance can be measured at a voltage determined by the battery potential of the ohmmeter and the resistance range at which the meter is set. When the test leads of the ohmmeter are connected to the diode, a resistance will be measured that is different from the resistance indicated if the leads are reversed. The smaller value is called the forWARD Resistance, and the larger value is called the BACK Resistance. If the ratio of back-to-forward resistance is greater than 10 to 1, the diode should be capable of functioning as a rectifier. However, keep in mind that this is a very limited test that does not take into account the action of the diode at voltages of different magnitudes and frequencies. (Note: This test should never be used to test crystal mixer diodes in radars. It will destroy their sensitivity.)

An oscilloscope can be used to graphically display the back-and-forward resistance characteristics of a crystal diode. a circuit used in conjunction with an oscilloscope to make this test is shown in figure 2- 15. This circuit uses the oscilloscope line-test voltage as the test signal. a series circuit (composed of resistor R1 and the internal resistance in the line-test circuit) decreases a 3-volt, open-circuit test voltage to a value of approximately 2 volts peak to peak.

Module 16 - Introduction to Test EquipmentNavy Electricity and Electronics Training Series (NEETS)Chapter 2: Pages 2-11 through 2-20

Module 16 - Introduction to Test Equipment
Navy Electricity and Electronics Training Series (NEETS)
Chapter 2: Pages 2-11 through 2-20