NEETS Module 9 — Introduction to Wave- Generation and Wave-Shaping
i - ix
, 1-1 to 1-10
1-11 to 1-20
, 1-21 to 1-30
1-31 to 1-40
,1-41 to 1-52
2-1 to 2-10
, 2-11 to 2-20
2-21 to 2-30
, 2-31 to 2-38
3-1 to 3-10
, 3-11 to 3-20
3-21 to 3-30
, 3-31 to 3-40
3-41 to 3-50
,3-51 to 3-56
4-1 to 4-10
, 4-11 to 4-20
4-21 to 4-30
, 4-31- to 4-40
4-41 to 4-50
, 4-51 to 4-61
COMPOSITION OF NONSINUSOIDAL WAVES
Pure sine waves are basic wave shapes from which
other wave shapes can be constructed. Any waveform that is not a pure sine wave consists of two or more sine
waves. Adding the correct frequencies at the proper phase and amplitude will form square waves, sawtooth waves,
and other nonsinusoidal waveforms.
A waveform other than a sine wave is called a COMPLEX WAVE. You will
see that a complex wave consists of a fundamental frequency plus one or more HARMONIC frequencies. The shape of a
nonsinusoidal waveform is dependent upon the type of harmonics present as part of the waveform, their relative
amplitudes, and their relative phase relationships. In general, the steeper the sides of a waveform, that is, the
more rapid its rise and fall, the more harmonics it contains.
The sine wave which has the lowest frequency
in the complex periodic wave is referred to as the FUNDAMENTAL FREQUENCY. The type and number of harmonics
included in the waveform are dependent upon the shape of the waveform. Harmonics have two classifications — EVEN
numbered and ODD numbered. Harmonics are always a whole number of times higher than the fundamental frequency and
are designated by an integer (whole number). For example, the frequency twice as high as the fundamental frequency
is the SECOND HARMONIC (or the first even harmonic).
View (A) of figure 4-25 compares a square wave with sine waves. Sine wave K is the same frequency as the square
wave (its fundamental frequency). If another sine wave (L) of smaller amplitude but three times the frequency
(referred to as the third harmonic) is added to sine wave K, curve M is produced. The addition of these two
waveforms is accomplished by adding the instantaneous values of both sine waves algebraically. Curve M is called
the resultant. Notice that curve M begins to assume the shape of a square wave. Curve M is shown again in view
Figure 4-25.—Harmonic composition of a square wave.
As shown in view (B), when the fifth harmonic (curve N with its decreased amplitude) is added, the sides of the
new resultant (curve P) are steeper than before. In view (C), the addition of the seventh harmonic (curve Q),
which is of even smaller amplitude, makes the sides of the composite waveform (R) still steeper. The addition of
more odd harmonics will bring the composite waveform nearer the shape of the perfect square wave. A perfect square
wave is, therefore, composed of an infinite number of odd harmonics. In the composition of square waves, all the
odd harmonics cross the reference line in phase with the fundamental.
A sawtooth wave, shown in figure
4-26, is made up of both even and odd harmonics. Notice that each higher harmonic is added in phase as it crosses
the 0 reference in view (A), view (B), view (C), and view (D). The resultant, shown in view (D), closely resembles
a sawtooth waveform.
Figure 4-26A.—Composition of a sawtooth wave.
Figure 4-26B.—Composition of a sawtooth wave.
Figure 4-26C.—Composition of a sawtooth wave.
Figure 4-26D.—Composition of a sawtooth wave.
Figure 4-27 shows the composition of a peaked wave. Notice how the addition of each odd harmonic makes the peak
of the resultant higher and the sides steeper. The phase relationship between the harmonics of the peaked wave is
different from the phase relationship of the harmonics in the composition of the square wave. In the composition
of the square wave, all the odd harmonics cross the
reference line in phase with the fundamental. In the peaked wave, harmonics such as the third, seventh, and so
forth, cross the reference line 180 degrees out of phase with the fundamental; the fifth, ninth, and so forth,
cross the reference line in phase with the fundamental.
Figure 4-27.—Composition of a peaked wave.
Q15. What is the harmonic composition of a square wave?
Q16. What is the peaked
wave composed of?
Q17. What is the fundamental difference between the phase relationship of
the harmonics of the square wave as compared to the harmonics of a peaked wave?
Voltages Applied to an RC Circuit
The harmonic content of a square wave must be complete to
produce a pure square wave. If the harmonics of the square wave are not of the proper phase and amplitude
relationships, the square wave will not be pure. The term PURE, as applied to square waves, means that the
waveform must be perfectly square.
Figure 4-28 shows a pure square wave that is applied to a
series-resistive circuit. If the values of the two resistors are equal, the voltage developed across each resistor
will be equal; that is, from one pure square-wave input, two pure square waves of a lower amplitude will be
produced. The value of the resistors does not affect the phase or amplitude relationships of the harmonics
contained within the square waves. This is true because the same opposition is offered by the resistors to all the
harmonics presented. However, if the same square wave is applied to a series RC circuit, as shown in figure 4-29,
the circuit action is not the same.
Figure 4-28.—Square wave applied to a resistive circuit.
Figure 4-29.—Square wave applied to an RC circuit.
The RC INTEGRATOR is used as a waveshaping network in communications,
radar, and computers. The harmonic content of the square wave is made up of odd multiples of the fundamental
frequency. Therefore SIGNIFICANT HARMONICS (those that have an effect on the circuit) as high as 50 or 60 times
the fundamental frequency will be present in the wave. The capacitor will offer a reactance (XC) of a
different magnitude to each of the harmonics
This means that the voltage drop across the capacitor for each harmonic frequency present will not be the same.
To low frequencies, the capacitor will offer a large opposition, providing a large voltage drop across the
capacitor. To high frequencies, the reactance of the capacitor will be extremely small, causing a small voltage
drop across the capacitor. This is no different than was the case for low- and high- pass filters (discriminators)
presented in chapter 1. If the voltage component of the harmonic is not developed across the reactance of the
capacitor, it will be developed across the resistor, if we observe Kirchhoff's voltage law. The harmonic amplitude
and phase relationship across the capacitor is not the same as that of the original frequency input; therefore, a
perfect square wave will not be produced across the capacitor. You should remember that the reactance offered to
each harmonic frequency will cause a change in both the amplitude and phase of each of the individual harmonic
frequencies with respect to the current reference. The amount of phase and amplitude change taking place across
the capacitor depends on the XC of the capacitor. The value of the resistance offered by the
resistor must also be considered here; it is part of the ratio of the voltage development across the network.
The circuit in figure 4-30 will help show the relationships of R and XC more clearly. The square
wave applied to the circuit is 100 volts peak at a frequency of 1 kilohertz. The odd harmonics will be 3
kilohertz, 5 kilohertz, 7 kilohertz, etc. Table 4-1 shows the values of XC and R offered to
harmonics and indicates the approximate value of the cutoff frequency (XC = R). The
table clearly shows that the cutoff frequency lies between the fifth and seventh harmonics. Between these two
values, the capacitive reactance will equal the resistance. Therefore, for all harmonic frequencies above the
fifth, the majority of the output voltage will not be developed across the output capacitor. Rather, most of the
output will be developed across R. The absence of the higher order harmonics will cause the leading edge of the
waveform developed across the capacitor to be rounded. An example of this effect is shown in figure 4-31. If the
value of the capacitance is increased, the reactances to each harmonic frequency will be further decreased. This
means that even fewer harmonics will be developed across the capacitor.
Figure 4-30.—Partial integration circuit.
Figure 4-31.—Partial integration.
Table 4-1.—Resistive and reactive values
The harmonics not effectively developed across the capacitor must be developed across the resistor to satisfy
Kirchhoff's voltage law. Note the pattern of the voltage waveforms across the resistor and capacitor. If the
waveforms across both the resistor and the capacitor were added graphically, the resultant would be an exact
duplication of the input square wave.
When the capacitance is increased sufficiently, full integration of
the input signal takes place in the output across the capacitor. An example of complete integration is shown in
figure 4-32 (waveform eC). This effect can be caused by significantly decreasing the value of
capacitive reactance. The same effect would take place by increasing the value of the resistance. Integration
takes place in an RC circuit when the output is taken across the capacitor.
The amount of integration is dependent upon the values of R and C. The amount of integration may also
be dependent upon the time constant of the circuit. The time constant of the circuit should be at least 10 TIMES
GREATER than the time duration of the input pulse for integration to occur. The value of 10 is only an
approximation. When the time constant of the circuit is 10 or more times the value of the duration of the input
pulse, the circuit is said to possess a long time constant. When the time constant is long, the capacitor does not
have the ability to charge instantly to the value of the applied voltage. Therefore, the result is the long,
sloping, integrated waveform.
Q18. What are the requirements for an integration circuit?
Q19. Can a pure sine
wave be integrated? Why?
The RL circuit may also be used as an
integrating circuit. An integrated waveform may be obtained from the series RL circuit by taking the output across
the resistor. The characteristics of the inductor are such that at the first instant of time in which voltage is
applied, current flow through the inductor is minimum and the voltage developed across it is maximum. Therefore,
the value of the voltage drop across the series resistor at that first instant must be 0 volts because there is no
current flow through it. As time passes, current begins to flow through the circuit and voltage develops across
the resistor. Since the circuit has a long time constant, the voltage across the resistor does NOT respond to the
rapid changes in voltage of the input square wave. Therefore, the conditions for integration in an RL circuit are
a long time constant with the output taken across the resistor. These conditions are shown in figure 4-33.
Figure 4-33.—RL integrator waveform.
Q20. What characteristic of an RL circuit allows it to act as an integrator?
INTEGRATOR WAVEFORM ANALYSIS
If either an RC or RL circuit has a time constant 10 times greater
than the duration of the input pulse, the circuits are capable of integration. Let's compute and graph the actual
waveform that would result
from a long time constant (10 times the pulse duration), a short time constant (1/10 of the pulse
duration), and a medium time constant (that time constant between the long and the short). To accurately plot
values for the capacitor output voltage, we will use the Universal Time Constant Chart shown in figure 4-34.
Figure 4-34.—Universal Time Constant Chart.
You already know that capacitor charge follows the shape of the curve shown in figure 4-34. This curve may be
used to determine the amount of voltage across either component in the series RC circuit. As long as the time
constant or a fractional part of the time constant is known, the voltage across either component may be
Short Time-Constant Integrator
In figure 4-35, a 100-microsecond pulse at an amplitude of
100 volts is applied to the circuit. The circuit is composed of the, 0.01µF capacitor and the variable resistor,
R. The square wave applied is a
pure square wave. The resistance of the variable resistor is set at a value of
1,000 ohms. The time constant of the circuit is given by the equation:
TC = RC
T = 1,000 · 0.01µF
T = (1 x 103) · (1 x -8)
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