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
T = 1 x 10-5 vor 10 microseconds
Figure 4-35.—RC integrator circuit.
Since the time constant of the circuit is 10 microseconds and the pulse duration is 100 microseconds, the time
constant is short (1/10 of the pulse duration). The capacitor is charged exponentially through the resistor. In 5
time constants, the capacitor will be, for all practical purposes, completely charged. At the first time constant,
the capacitor is charged to 63.2 volts, at the second 86.5 volts, at the third 95 volts, at the fourth 98 volts,
and finally at the end of the fifth time constant (50 microseconds), the capacitor is fully charged. This is shown
in figure 4-36.
Figure 4-36.—Square wave applied to a short time-constant integrator.
Notice that the leading edge of the square wave taken across the capacitor is rounded. If the time constant
were made extremely short, the rounded edge would become square.
Medium Time-Constant Integrator
The time constant, in figure 4-36 can be changed by increasing the value of the variable resistor
to 10,000 ohms. The time constant will then be equal to 100 microseconds.
This time constant is known as a
medium time constant. Its value lies between the extreme ranges of the short and long time constants. In this
case, its value happens to be exactly equal to the duration of the input pulse, 100 microseconds. The output
waveform, after several time constants, is shown in figure
4-37. The long, sloping rise and fall of voltage is caused by the inability of the capacitor to charge
and discharge rapidly through the 10,000-ohm series resistance.
Figure 4-37.—Medium time-constant integrator.
At the first instant of time, 100 volts is applied to the medium time-constant circuit. In this circuit, 1TC is
exactly equal to the duration of the input pulse. After 1TC the capacitor has charged to 63.2 percent of the input
voltage (100 volts). Therefore, at the end of 1TC (100 microseconds), the voltage across the capacitor is equal to
63.2 volts. However, as soon as 100 microseconds has elapsed, and the initial charge on the capacitor has risen to
63.2 volts, the input voltage suddenly drops to 0. It remains
there for 100 microseconds. The capacitor will
now discharge for 100 microseconds. Since the discharge time is 100 microseconds (1TC), the capacitor will
discharge 63.2 percent of its total 63.2-volt charge, a value of 23.3 volts. During the next 100 microseconds, the
input voltage will increase from 0 to 100 volts instantaneously. The capacitor will again charge for 100
microseconds (1TC). The voltage available for this charge is the difference between the voltage applied and the
charge on the capacitor (100 - 23.3 volts), or 76.7 volts. Since the capacitor will only be able to charge for
1TC, it will charge to 63.2 percent of the 76.7 volts, or 48.4 volts. The total charge on the capacitor at the end
of 300 microseconds will be 23.3 + 48.4 volts, or 71.7 volts.
Notice that the capacitor voltage at the end
of 300 microseconds is greater than the capacitor voltage at the end of 100 microseconds. The voltage at the end
of 100 microseconds is 63.2 volts, and the capacitor voltage at the end of 300 microseconds is 71.7 volts, an
increase of 8.5 volts.
The output waveform in this graph (eC) is the waveform that will be produced after
many cycles of input signal to the integrator. The capacitor will charge and discharge in a step-by-step manner
until it finally charges and discharges above and below a 50-volt level. The 50-volt level is controlled by the
maximum amplitude of the symmetrical input pulse, the average value of which is 50 volts.
If the resistance in the circuit of figure 4-35 is increased to 100,000 ohms, the time constant of the circuit
will be 1,000 microseconds. This time constant is 10 times the pulse duration of the input pulse. It is,
therefore, a long time-constant circuit.
The shape of the output waveform across the capacitor is shown in
figure 4-38. The shape of the output waveform is characterized by a long, sloping rise and fall of capacitor
Figure 4-38.—Square wave applied to a long time-constant integrator.
At the first instant of time, 100 volts is applied to the long time-constant circuit. The value of charge on
the capacitor at the end of the first 100 microseconds of the input signal can be found by using the Universal
Time Constant Chart (figure 4-34). Assume that a line is projected up from the point on the base line
corresponding to 0.1TC. The line will intersect the curve at a point that is the percentage of voltage across the
capacitor at the end of the first 100 microseconds. Since the applied voltage is 100 volts, the charge on the
capacitor at the end of the first 100 microseconds will be approximately 9.5 volts. At the end of the first 100
microseconds, the input signal will fall suddenly to 0 and the capacitor will begin to discharge. It will be able
to discharge for 100 microseconds. Therefore, the capacitor will discharge 9.5 percent of its accumulated 9.5
volts (.095 ´ 9.5 = 0.90 volt). The discharge of the 0.90 volt will result in a remaining charge on the capacitor
of 8.6 volts. At the end of 200 microseconds, the input signal will again suddenly rise to a value of 100 volts.
The capacitor will be able to charge to 9.5 percent of the difference (100 - 8.6 = 91.4 volts). This may also be
figured as a value of 8.7 volts plus the initial 8.6 volts. This results in a total charge on the capacitor (at
the end of the first 300 microseconds) of 8.7 + 8.6 = 17.3 volts.
Notice that the capacitor voltage at the end of the first 300 microseconds is greater than the capacitor voltage
at the end of the first 100 microseconds. The voltage at the end of the first 100 microseconds is 9.5 volts; the
capacitor voltage at the end of the first 300 microseconds is 17.3 volts, an increase of 7.8 volts.
capacitor charges and discharges in this step-by-step manner until, finally, the capacitor charges and discharges
above and below a 50-volt level. The 50-volt level is controlled by the maximum amplitude of the square-wave input
pulse, the average value of which is 50 volts.
Q21. What is the numerical difference (in terms
of the time constant) between a long and a short time- constant circuit?
Q22. What would
happen to the integrator output if the capacitor were made extremely large (all other factors remaining the same)?
DIFFERENTIATION is the direct opposite of integration. In the RC
integrator, the output is taken from the capacitor. In the differentiator, the output is taken across the
resistor. Likewise, this means that when the RL circuit is used as a differentiator, the differentiated output is
taken across the inductor.
An application of Kirchhoff's law shows the relationship between the waveforms across the resistor and
capacitor in a series network. Since the sum of the voltage drops in a closed loop must equal the total applied
voltage, the graphical sum of the voltage waveforms in a closed loop must equal the applied waveform. Figure 4-39
shows a differentiator circuit with the output taken across a variable resistor.
Figure 4-39.—RC circuit as a differentiator.
Short Time-Constant Differentiator
With the variable resistor set at 1,000 ohms and
the capacitor value of 0.01 microfarad, the time constant of the circuit is 10 microseconds. Since the input
waveform has a duration of 100 microseconds, the circuit is a short time-constant circuit.
At the first
instant of time in the short time-constant circuit, the voltage across the capacitor is 0. Current flows through
the resistor and causes a maximum voltage to be developed across it. This is shown at the first instant of time in
the graph of figure 4-40.
Figure 4-40.—Square wave applied to a short time-constant differentiator.
As the capacitor begins accumulating a charge, the voltage developed across the resistor will begin to
decrease. At the end of the first time constant, the voltage developed across the resistor will have decreased by
a value equal to 63.2 percent of the applied voltage. Since 100 volts is applied, the voltage across the resistor
after 1TC will be equal to 36.8 volts. After the second time constant, the voltage across the resistor will be
down to 13.5 volts. At the end of the third time constant, eR will be 5 volts and at the
end of the fourth time constant, 2 volts. At the end of the fifth time constant, the voltage across the
resistor will be very close to 0 volts. Since the time constant is equal to 10 microseconds, it will take a total
of 50 microseconds to completely charge the capacitor and stop current flow in the circuit.
As shown in
figure 4-40 the slope of the charge curve will be very sharp. The voltage across the resistor will remain at 0
volts until the end of 100 microseconds. At that time, the applied voltage suddenly drops to 0, and the capacitor
will now discharge through the resistor. At this time, the discharge current will be maximum causing a large
discharge voltage to develop across the resistor. This is shown as the negative spike in figure 4-40. Since the
current flow from the capacitor, which now acts like a source, is decreasing exponentially, the voltage across the
resistor will also decrease. The resistor voltage will decrease exponentially to 0 volts in 5 time constants. All
of this discharge action will take a total of 50 microseconds. The discharge curve is also shown in figure 4-40.
At the end of 200 microseconds, the action begins again. The output waveform taken across the resistor in this
short time-constant circuit is an example of differentiation. With the square wave applied, positive and negative
spikes are produced in the output. These spikes approximate the rate of change of the input square wave.
Medium Time-Constant Differentiator
The output across the resistor in an RC circuit of a medium time constant is shown in figure 4-41. The value of
the variable resistor has been increased to a value of 10,000 ohms. This means that the time constant of the
circuit is equal to the duration of the input pulse or 100 microseconds. For clarity, the voltage waveforms
developed across both the resistor and the capacitor are shown. As before, the sum of the voltages across the
resistor and capacitor must be equal to the applied voltage of 100 volts.
Figure 4-41.—Voltage outputs in a medium time-constant differentiator.
At the first instant of time, a pulse of 100 volts in amplitude with a duration of 100 microseconds is applied.
Since the capacitor cannot respond quickly to the change in voltage, all of the applied voltage is felt across the
resistor. Figure 4-41 shows the voltage across the resistor (eR) to be 100 volts and the voltage across
the capacitor (eC) to be 0 volts. As time progresses, the capacitor charges. As the capacitor voltage
increases, the resistor voltage decreases. Since the time that the capacitor is permitted to charge is 100
microseconds (equal to 1TC in this circuit), the capacitor will charge to 63.2 percent of the applied
voltage at the end of 1TC, or 63.2 volts. Because Kirchhoff's law must be followed at all times, the
voltage across the resistor must be equal to the difference between the applied voltage and the charge on the
capacitor (100 - 63.2 volts), or 36.8 volts.
At the end of the first 100 microseconds, the input voltage
suddenly drops to 0 volts. The charge on the capacitor (-63.2 volts) becomes the source and the entire voltage is
developed across the resistor for the first instant.
The capacitor discharges during the next 100
microseconds. The voltage across the resistor decreases at the same rate as the capacitor voltage and total
voltage is maintained at 0. This exponential decrease in resistor voltage is shown during the second 100
microseconds in figure 4-41. The capacitor will discharge 63.2 percent of its charge to a value of 23.3 volts at
the end of the second 100 microseconds. The resistor voltage will rise in the positive direction to a value of
-23.3 volts to maintain the total voltage at 0 volts.
At the end of 200 microseconds, the input voltage
again rises suddenly to 100 volts. Since the capacitor cannot respond to the 100-volt increase instantaneously,
the 100-volt change takes place across the resistor. The voltage across the resistor suddenly rises from -23.3
volts to +76.7 volts. The capacitor will now begin to charge for 100 microseconds. The voltage will decrease
across the resistor. This charge and discharge action will continue for many cycles. Finally, the voltage across
the capacitor will rise and fall by equal amounts both above and below about a 50-volt level. The resistor voltage
will also rise and fall by equal amounts to about a 0-volt level.
Long Time-Constant Differentiator
If the time constant for the circuit in figure 4-39 is
increased to make it a long time-constant circuit, the differentiator output will appear more like the input. The
time constant for the circuit can be changed by either increasing the value of capacitance or resistance. In this
circuit, the time constant will be increased by increasing the value of resistance from 10,000 ohms to 100,000
ohms. Increasing the value of resistance will result in a time constant of 1,000 microseconds. The time constant
is 10 times the duration of the input pulse. The output of this long time-constant circuit is shown in figure
Figure 4-42.—Voltage outputs in a long time-constant differentiator.
At the first instant of time, a pulse of 100-volts amplitude with a duration of 100 microseconds is
applied. Since the capacitor cannot respond instantaneously to a change in voltage, all of the applied voltage is
felt across the resistor. As time progresses, the capacitor will charge and the voltage across the resistor will
be reduced. Since the time that the capacitor is permitted to charge is 100 microseconds, the capacitor will
charge for only 1/10 of 1TC or to 9.5 percent of the applied voltage. The voltage across the resistor must be
equal to the difference between the applied voltage and the charge on the capacitor (100 - 9.5 volts), or 90.5
At the end of the first 100 microseconds of input, the applied voltage suddenly drops to 0 volts, a
change of 100 volts. Since the capacitor is not able to respond to so rapid a voltage change, it becomes the
source of 9.5 volts. This causes a -9.5 voltage to be felt across the resistor in the first instant of time. The
sum of the voltage across the two components is now 0 volts.
During the next 100 microseconds, the
capacitor discharges. The total circuit voltage is maintained at 0 by the voltage across the resistor decreasing
at exactly the same rate as the capacitor discharge. This exponential decrease in resistor voltage is shown during
the second 100 microseconds of operation. The capacitor will now discharge 9.5 percent of its charge to a value of
8.6 volts. At the end of the second 100 microseconds, the resistor voltage will rise in a positive direction to a
value of -8.6 volts to maintain the total circuit voltage at 0 volts.
At the end of 200 microseconds, the input voltage again suddenly rises to 100 volts. Since the capacitor cannot
respond to the 100-volt change instantaneously, the 100-volt change takes place across the resistor. This
step-by-step action will continue until the circuit stabilizes. After many cycles have passed, the capacitor
voltage varies by equal amounts above and below the 50-volt level. The resistor voltage varies by equal amounts
both above and below a 0-volt level.
The RC networks which have been discussed in this chapter may also be used as coupling networks. When an RC
circuit is used as a coupling circuit, the output is taken from across the resistor. Normally, a long
time-constant circuit is used. This, of course, will cause an integrated wave shape across the capacitor if the
applied signal is nonsinusoidal. However, in a coupling circuit, the signal across the resistor should closely
resemble the input signal and will if the time constant is sufficiently long. By referring to the diagram in
figure 4-42, you can see that the voltage across the resistor closely resembles the input signal. Consider what
would happen if a pure sine wave were applied to a long time-constant RC circuit (R is much greater than XC).
A large percentage of the applied voltage would be developed across the resistor and only a small amount across
Q23. What is the difference between an RC and an RL differentiator in terms of
where the output is developed?
A counting circuit receives uniform pulses representing units to be counted. It
provides a voltage that is proportional to the frequency of the units.
With slight modification, the
counting circuit can be used with a blocking oscillator to produce trigger pulses which are a submultiple of the
frequency of the pulses applied. In this case the circuit acts as a frequency divider.
The pulses applied
to the counting circuit must be of the same time duration if accurate frequency division is to be made. Counting
circuits are generally preceded by shaping circuits and limiting circuits (both discussed in this chapter) to
ensure uniformity of amplitude and pulse width. Under those conditions, the pulse repetition frequency is the only
variable and frequency variations may be measured.
Q24. Name a common application of counting circuits.
The POSITIVE-DIODE COUNTER circuit is used in timing or counting
circuits in which the number of input pulses are represented by the output voltage. The output may indicate
frequency, count the rpm of a shaft, or register a number of operations. The counter establishes a direct
relationship between the input frequency and the average dc output voltage. As the input frequency increases, the
output voltage also increases; conversely, as the input frequency decreases, the output voltage decreases. In
effect, the positive counter counts the number of positive input pulses by producing an average dc output voltage
proportional to the repetition frequency of the input signal. For accurate counting, the pulse repetition
frequency must be the only variable parameter in the input signal. Therefore, careful shaping and limiting of the
input signal is essential for you to ensure that the pulses are of uniform width and that the amplitude is
constant. When properly filtered and smoothed, the dc output voltage of the counter may be used to operate a
direct reading indicator.
Solid-state and electron-tube counters operate in manners similar to each other.
The basic solid-state (diode) counter circuit is shown in view (A) of figure 4-43. Capacitor C1 is the input
coupling capacitor. Resistor R1 is the load resistor across which the output voltage is developed. For the purpose
of circuit discussion, assume that the input pulses (shown in view (B)) are of constant amplitude and time
duration and that only the pulse repetition frequency changes. At time T0, the positive-going input pulse is
applied to C1 and causes the anode of D2 to become positive. D2 conducts and current ic flows
through R1 and D2 to charge C1. Current ic, develops an output voltage across R1, shown as eout.
Figure 4-43A.—Positive-diode counter and waveform.
Figure 4-43B.—Positive-diode counter and waveform.
The initial heavy flow of current produces a large voltage across R1 which tapers off exponentially as C1
charges. The charge on C1 is determined by the time constant of R1 and the conducting resistance of the diode
times the capacitance of C1. For ease of explanation, assume that C1 is charged to the peak value before T1.
At T1 the input signal reverses polarity and becomes negative-going. Although the charge on capacitor C1 cannot
change instantly, the applied negative voltage is equal to or greater than the charge on C1. This causes the anode
of D2 to become negative and conduction ceases. When D2 stops conducting eout is at 0. C1 quickly
discharges through D1 since its cathode is now negative with respect to ground. Between T1 and T2 the input pulse
is again at the 0-volt level and D2 remains in a nonconducting state. Since the very short time constant provided
by the conduction resistance of D1 and C1 is so much less than the long time constant offered by D2 and R1 during
the conduction period, C1 is always completely discharged between pulses. Thus, for each input pulse, a precise
level of charge is deposited on C1. For each charge of C1 an identical output pulse is produced by the flow of ic
through R1. Since this current flow always occurs in the direction indicated by the solid arrow, the dc output
voltage is positive.
At T2 the input signal again becomes positive and the cycle repeats. The time
duration between pulses is the interval represented by the period between T1 and T2 or between T3 and T4. If the
input- pulse frequency is reduced, these time periods become longer. On the other hand, if the frequency is
increased, these time intervals become shorter. With shorter periods, more pulses occur in a given length of time
and a higher average dc output voltage is produced; with longer periods, fewer pulses occur and a lower average dc
output voltage is produced. Thus, the dc output is directly proportional to the repetition frequency of the input
pulses. If the current and voltage are sufficiently large, a direct-reading meter can be used to indicate the
count. If they are not large enough to actuate a meter directly, a dc amplifier may be added. In the latter case,
a pi-type filter network is inserted at the output of R1 to absorb the instantaneous pulse variations and produce
a smooth direct current for amplification.
From the preceding discussion, you should see that the voltage
across the output varies in direct proportion to the input pulse repetition rate. Hence, if the repetition rate of
the incoming pulses increases, the voltage across R1 also increases. For the circuit to function as a frequency
counter, some method must
be employed to use this frequency-to-voltage relationship to operate an indicator. The block diagram in
view (A) of figure 4-44 represents one simple circuit which may be used to perform this function. In this circuit,
the basic counter is fed into a low-pass filter and an amplifier with a meter that is calibrated in units of
Figure 4-44.—Basic frequency counter.
A typical schematic diagram is shown in view (B). The positive pulses from the counter are filtered by C2, R2,
and C3. The positive dc voltage from the filter is applied to the input of amplifier A. This voltage increases
with frequency; as a consequence, the current through the device increases. Since emitter or cathode current flows
through M1, an increase in amplifier current causes an increase in meter deflection. The meter may be calibrated
in units of time, frequency, revolutions per minute, or any function based upon the relationship of output voltage
to input frequency.
Q25. What establishes the value of the current that flows in the output of
Q26. What is the purpose of D1 in figure 4-43?
Reversing the connections of diodes D1 and D2 in the positive-counter circuit (view (A) of figure 4- 43) will
cause the circuit to respond to negative pulses and become a negative-counter circuit. Diode D2 conducts during
the time the negative pulse is applied and current flows in the opposite direction through R1, as was indicated by
the arrow. At the end of the negative pulse, D1 conducts and discharges C1. The current through R1 increases with
an increase in pulse frequency as before. However, if the voltage developed across R1 is applied to the same
control circuit, as shown in view (A) of figure 4-44, the increase in current will be in a negative direction and
the amplifier will conduct less. Thus, the effect is opposite to that of the positive counter.
Step-by-Step (Step) Counters
The STEP-BY-STEP (STEP) COUNTER is used as a voltage multiplier when
a stepped voltage must be provided to any device which requires such an input. The step counter provides an output
which increases in one-step increments for each cycle of the input. At some predetermined level, the output
voltage reaches a point which causes a circuit, such as a blocking oscillator, to be triggered.
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