NEETS Module 9 — Introduction to Wave- Generation and Wave-Shaping
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, 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
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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
A schematic diagram of a positive step counter is shown in view (A) of figure 4-45. For step counting, the load
resistor of the positive-counting circuit is replaced by capacitor C2. This capacitor is relatively large in
comparison to C1. Each time D2 conducts, the charge on C2 increases as shown in view (B). The steps are not the
same height each time. They decrease exponentially with time as the voltage across C2 approaches the input
Figure 4-45A.—Basic step counter and waveforms.
Figure 4-45B.—Basic step counter and waveforms.
As long as C2 has no discharge path, the voltage across its terminals increases with each successive step until
it is equal in amplitude to the applied pulse. The voltage across C2 could be applied to a blocking-oscillator
circuit to cause the oscillator to pulse after a certain amount of voltage is applied to it.
in figure 4-46, (view A) and (view B), may be used as a frequency divider. When used in this manner, Q1 is used as
a single-swing blocking oscillator that is triggered when the voltage across C2 becomes great enough to forward
bias Q1. At other times, the transistor is cut off by the bias voltage developed in the section of R2 that is
between the ground and the slide.
Figure 4-46A.—Step counter as a frequency divider and waveforms.
Figure 4-46B.—Step counter as a frequency divider and waveforms.
The action of the counter can best be understood by referring back to figure 4-45. Assume C2 is 10 times larger
than C1 and the peak voltage is 10 volts. C1 will assume 9/10 of the positive input voltage at T0, while C2 will
assume only 1/10, or 1 volt in this example. At T1 the input will drop in a negative direction and D2 will be cut
off. The cathode of D1 will become more negative than its anode and conduct, discharging C1. The charge on C2 will
remain at 1 volt because it has no discharge path. At T2 the second pulse will be applied. The 1-volt charge on C2
will oppose the 10 volts of the second pulse, and the applied voltage for the capacitors to charge will be 9
volts. C2 will again charge 10 percent, or 0.9 volt. This is in addition to the initial charge of volt. At the end
of the second pulse, the voltage on C2 will be 1.9 volts. At T3 the third pulse will be 10 volts, but 1.9 volts
will oppose it. Therefore, the applied
voltage will be 10 - 1.9 volts, or 8.1 volts. C2 will charge to 10 percent of 8.1 volts, or .81 volt.
The voltage on C2 will become 1 + .9 + .81, or 2.71 volts. Successive input pulses will raise C2 by 10 percent of
the remaining voltage toward 10 volts until the blocking oscillator works. If the oscillator bias is set so that
Q1 begins conduction at 3.8 volts, this will continue until 3.8 volts is exceeded. Since the fourth step is 3.5
volts and the fifth is 4.1 volts, the 3.8-volt level is crossed at the fifth step. If the oscillator goes through
1 cycle of operation every fifth step and C2 is discharged at this point, this circuit would be a 5- to-1 divider.
The circuit can be made to divide by 3, 4, or some other value by setting the bias at a different level. For
example, if the bias is set at 2.9 volts, conduction will occur at the fourth step, making it a 4-to-1 divider.
The counting stability of the step counter is dependent upon the exponential charging rate of capacitor C2.
As C2 increases to higher steps, the voltage increments are less and less. If the ratio becomes too great, the
higher steps become almost indiscernible. For this reason, accuracy decreases as the ratio increases. When you
desire to count by a large number, 24 for example, a 6-to-1 counter and a 4- to-1 counter are connected in cascade
(series). A more stable method of counting 24 would be to use a 2:1, 3:1, 4:1 counter connected in cascade. Most
step counters operate on a ratio of 5 to 1 or less.
Q27. What is the difference between a
positive counter and a step counter?
This chapter has presented information on wave shaping. The information that follows summarizes the important
points of this chapter.
A LIMITER is a device which limits or prevents some part of a
waveform from exceeding a specified value.
In a SERIES LIMITER, the diode is in series
with the output. It can limit either the negative or positive alternation of the input signal.
SERIES-POSITIVE LIMITER, the diode is in series with the output which is taken across the resistor. It
removes the positive alternation of the input signal.
In a SERIES-POSITIVE LIMITER WITH BIAS, the bias potential will either aid or oppose the flow
of current. When aiding forward bias, only a portion of the positive input pulse is removed. When the bias aids
the reverse bias, all of the positive and a portion of the negative pulse is removed.
The SERIES-NEGATIVE LIMITER limits the negative portion of the input pulse. The difference
between a series-negative limiter and a series-positive limiter is that the diode is reversed in the negative
A SERIES-NEGATIVE LIMITER with bias is the same as the series-positive limiter with bias, but
the outputs are opposite. When bias aids forward bias, only a portion of the negative input is removed. When bias
aids reverse bias, all of the negative and a portion of the positive input is removed.
In a PARALLEL LIMITER, a resistor and diode are connected in series with the input signal. The
output is taken across the diode.
In the PARALLEL-POSITIVE LIMITER, the positive portion
of the input signal is limited when the diode conducts.
The PARALLEL-NEGATIVE LIMITER diode is reversed from that of the parallel positive limiter to
limit only a portion of the negative input signal.
The DUAL-DIODE LIMITER combines the parallel negative limiter with negative bias (reverse
bias) and the parallel positive limiter with positive bias (reverse bias). It will remove parts of the positive
and negative input signal.
A CLAMPING CIRCUIT effectively clamps or ties down the upper or lower extremity of a waveform
to a fixed dc potential. Clamping does not change the amplitude or shape of the input waveform.
A POSITIVE CLAMPER will clamp the lower extremity of the input waveform to a dc potential of
A NEGATIVE CLAMPER will clamp the upper extremity of the input waveform to a dc potential of 0
A COMMON-BASE TRANSISTOR CLAMPER clamps the collector voltage to a reference level. A waveform
other than a sine wave is called a COMPLEX WAVE.
If the odd harmonics of a sine wave are added algebraically,
the result is a square wave. A PERFECT SQUARE WAVE is composed of an infinite number of odd harmonics in phase
with the fundamental wave.
A SAWTOOTH WAVE is made up of different harmonics, both odd and even.
A PEAKED WAVE is made up of odd harmonics that are in phase and out of phase with the
INTEGRATION takes place in an RC circuit with the output taken across the capacitor. The
amount of integration is dependent upon the time constant of the circuit. Full integration takes place when the
time constant of the RC circuit is at least 10 times greater than the duration of the input pulse. An RL circuit
is also used as an integration circuit. The output is taken across the resistor and the time constant of the
circuit is 10 times greater than the input pulse.
DIFFERENTIATION is the opposite of integration. In the differentiator, the output is
taken across the resistor. Full differentiation takes place when the time constant of the circuit is 1/10 that of
the input pulse.
A COUNTING CIRCUIT receives uniform pulses, representing units to be counted, and produces a
voltage output proportional to its frequency.
ANSWERS TO QUESTION Q1. THROUGH Q27.
A4. The diode.
A5. Conducting, cutoff.
A6. Short time
A7. Long time constant.
A8. Most negative.
A9. Positive potential.
A10. Positive clamper with negative bias.
A11. Most positive.
A12. Negative potential.
A14. -5 volts.
A15. It is composed of an infinite number of odd harmonics in phase with the fundamental.
A16. It is composed of odd harmonics some of which are out phase with the fundamental.
All the odd harmonics are in phase with the fundamental in the square wave. This is not true of the odd harmonics
in the peaked wave.
A18. The time constant is long and the output is taken across the
capacitor in an RC circuit.
A19. A pure sine wave cannot be integrated; it contains no
A20. The ability of the inductor to oppose a change in current.
time-constant value of a long time constant-circuit is 10 times the value of the input pulse duration. The short
time-constant circuit has a time constant of 1/10 of the pulse duration.
A22. A more complete
integration of the waveform would result from the long time constant.
A23. In an RC circuit
the output is taken across the resistor. In the RL circuit the output is taken across the inductor.
Frequency counters or frequency dividers.
A25. The frequency of the voltage input.
A26. To provide a quick discharge path for C1.
A27. The load resistor in a
positive counter is replaced by a capacitor in a step counter.
Introduction to Matter, Energy, and Direct Current, Introduction
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,
Modulation Principles, Introduction to Number Systems and Logic Circuits, Introduction
to Microelectronics, Principles of Synchros, Servos, and Gyros,
Introduction to Test Equipment, Radio-Frequency
Communications Principles, Radar Principles, The Technician's Handbook,
Master Glossary, Test Methods and Practices, Introduction to Digital Computers,
Magnetic Recording, Introduction to Fiber Optics