Module 8—Introduction to Amplifiers
CHAPTER 2 VIDEO AND RF
Pages i - ix
1-1 to 1-10
, 1-11 to 1-20
1-21 to 1-30
, 1-31 to 1-40
2-1 to 2-10
, 2-11 to 2-20
2-21 to 2-30
, 2-31 to 2-35
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 3-60
3-61 to 3-70
, AI-1 to AI-3
Upon completion of this chapter, you will be able to:
1. Define the term "bandwidth of an
2. Determine the upper and lower frequency limits of an amplifier from a frequency-response
3. List the factors that limit frequency response in an amplifier.
4. List two
techniques used to increase the high-frequency response for a video amplifier.
5. State one technique
used to increase the low-frequency response of a video amplifier.
6. Identify the purpose of various
components on a schematic of a complete typical video amplifier circuit.
7. State the purpose of a
frequency-determining network in an RF amplifier.
8. State one method by which an RF amplifier can be
9. Identify the purpose of various components on a schematic of a complete typical RF amplifier.
In this chapter you will be given information on the frequency response of amplifiers as well as
specific information on video and RF amplifiers. For all practical purposes, all the general information you
studied in chapter 1 about audio amplifiers will apply to the video and RF amplifiers which you are about to
You may be wondering why you need to learn about video and RF amplifiers. You need to understand
these circuits because, as a technician, you will probably be involved in working on equipment in which these
circuits are used. Many of the circuits shown in this and the next chapter are incomplete and would not be used in
actual equipment. For example, the complete biasing network may not be shown. This is done so you can concentrate
on the concepts being presented without being overwhelmed by an abundance of circuit elements. With this idea in
mind, the information that is presented in this chapter is real, practical information about video and RF
amplifiers. It is the sort of information that you will use in working with these circuits. Engineering
information (such as design specifications) will not be presented because it is not needed to understand the
concepts that a technician needs to perform the job of circuit analysis and repair. Before you are given the
specific information on video and RF amplifiers, you may be wondering how these circuits are used.
amplifiers are used to amplify signals that represent video information. (That’s where the term "video" comes
from.) Video is the "picture" portion of a television signal. The "sound" portion is audio.
Although the Navy uses television in many ways, video signals are used for more than television. Radar
systems (discussed later in this training series) use video signals and, therefore, video amplifiers. Video
amplifiers are also used in video recorders and some communication and control devices. In addition to using video
amplifiers, televisions use RF amplifiers. Many other devices also use RF amplifiers, such as radios, navigational
devices, and communications systems. Almost any device that uses broadcast, or transmitted, information will use
an RF amplifier.
As you should recall, RF amplifiers are used to amplify signals between 10 kilohertz (10 kHz) and 100,000
megahertz (100,000 MHz) (not this entire band of frequencies, but any band of frequencies within these limits).
Therefore, any device that uses frequencies between 10 kilohertz and 100,000 megahertz will most likely use an RF
Before you study the details of video and RF amplifiers, you need to learn a little more about the frequency
response of an amplifier and frequency-response curves.
AMPLIFIER FREQUENCY RESPONSE
In chapter 1 of this module you were shown the frequency-response curve of an audio amplifier. Every
amplifier has a frequency-response curve associated with it. Technicians use frequency-response curves because
they provide a "picture" of the performance of an amplifier at various frequencies. You will probably never have
to draw a frequency-response curve, but, in order to use one, you should know how a frequency-response curve is
created. The amplifier for which the frequency-response curve is created is tested at various frequencies. At each
frequency, the input signal is set to some predetermined level of voltage (or current). This same voltage (or
current) level for all of the input signals is used to provide a standard input and to allow evaluation of the
output of the circuit at each of the frequencies tested. For each of these frequencies, the output is measured and
marked on a graph. The graph is marked "frequency" along the horizontal axis and "voltage" or "current" along the
vertical axis. When points have been plotted for all of the frequencies tested, the points are connected to form
the frequency-response curve. The shape of the curve represents the frequency response of the amplifier.
Some amplifiers should be "flat" across a band of frequencies. In other words, for every frequency within the
band, the amplifier should have equal gain (equal response). For frequencies outside the band, the amplifier gain
will be much lower.
For other amplifiers, the desired frequency response is different. For example,
perhaps the amplifier should have high gain at two frequencies and low gain for all other frequencies. The
frequency-response curve for this type of amplifier would show two "peaks." In other amplifiers the
frequency-response curve will have one peak indicating high gain at one frequency and lower gain at all others.
Note the frequency-response curve shown in figure 2-1. This is the frequency-response curve for an audio
amplifier as described in chapter 1. It is "flat" from 15 hertz (15 Hz) to 20 kilohertz (20 kHz).
Figure 2-1.—Frequency response curve of audio amplifier.
Notice in the figure that the lower frequency limit is labeled f1 and the upper frequency limit is
labeled f2. Note also the portion inside the frequency-response curve marked "BANDWIDTH." You may be wondering
just what a "bandwidth" is. BANDWIDTH OF AN AMPLIFIER
The bandwidth represents the amount or "width" of frequencies, or the "band of frequencies," that the amplifier is
MOST effective in amplifying. However, the bandwidth is NOT the same as the band of frequencies that is amplified.
The bandwidth (BW) of an amplifier is the difference between the frequency limits of the amplifier. For example,
the band of frequencies for an amplifier may be from 10 kilohertz (10 kHz) to 30 kilohertz (30 kHz). In this case,
the bandwidth would be 20 kilohertz (20 kHz). As another example, if an amplifier is designed to amplify
frequencies between 15 hertz (15 Hz) and 20 kilohertz (20 kHz), the bandwidth will be equal to 20 kilohertz minus
15 hertz or 19,985 hertz (19,985 Hz). This is shown in figure 2-1.
You should notice on the figure that the frequency-response curve shows output voltage (or current)
against frequency. The lower and upper frequency limits (f1 and f2) are also known as HALF-POWER POINTS. The
half-power points are the points at which the output voltage (or current) is 70.7 percent of the maximum output
voltage (or current). Any frequency that produces less than 70.7 percent of the maximum output voltage (or
current) is outside the bandwidth and, in most cases, is not considered a useable output of the amplifier.
The reason these points are called "half-power points" is that the true output power will be half (50 percent) of
the maximum true output power when the output voltage (or current) is 70.7 percent of the maximum output voltage
(or current), as shown below. (All calculations are rounded off to two decimal places.)
As you learned in
NEETS, Module 2, in an a.c. circuit true power is calculated using the resistance (R) of the circuit, NOT the
impedance (Z). If the circuit produces a maximum output voltage of 10 volts across a 50-ohm load, then:
When the output voltage drops to 70.7 percent of the maximum voltage of 10 volts, then:
As you can see, the true power is 50 percent (half) of the maximum true power when the output voltage is
70.7 percent of the maximum output voltage. If, instead, you are using the output current of the above circuit,
the maximum current is
The calculations are:
At 70.7 percent of the output current (.14 A):
On figure 2-1, the two points marked f 1 and f2 will enable you to determine the frequency-response
limits of the amplifier. In this case, the limits are 15 hertz (15 Hz) and 20 kilohertz (20 kHz). You should now
see how a frequency-response curve can enable you to determine the frequency limits and the bandwidth of an
READING AMPLIFIER FREQUENCY-RESPONSE CURVES
Figure 2-2 shows the
frequency-response curves for four different amplifiers. View (A) is the same frequency-response curve as shown in
figure 2-1. View (B) is the frequency-response curve of an amplifier that would also be classified as an audio
amplifier, even though the curve is not "flat" from 15 hertz to 20 kilohertz and does not drop off sharply at the
frequency limits. From the curve, you can see that the lower frequency limit of this amplifier (f1) is 100 hertz.
The upper frequency limit (f2) is 10 kilohertz. Therefore, the bandwidth of this amplifier must be 10 kilohertz
minus 100 hertz or 9900 hertz. Most amplifiers will have a frequency-response curve shaped like view (B) if
nothing is done to modify the frequency-response characteristics of the circuit. (The factors that affect
frequency response and the methods to modify the frequency response of an amplifier are covered a little later in
Figure 2-2A.—Frequency response curves.
Figure 2-2B.—Frequency response curves.
Figure 2-2C.—Frequency response curves.
Figure 2-2D.—Frequency response curves.
Now look at view (C). This frequency-response curve is for an RF amplifier. The frequency limits
of this amplifier are 100 kilohertz (f1) and 1 megahertz (f2); therefore, the bandwidth of this amplifier is 900
View (D) shows another audio amplifier. This time the frequency limits are 30 hertz (f1) and
200 hertz (f2). The bandwidth of this amplifier is only 170 hertz. The important thing to notice in view (D) is
that the frequency scale is different from those used in other views. Any frequency scale can be used for a
frequency-response curve. The scale used would be determined by what frequencies are most useful in presenting the
frequency-response curve for a particular amplifier.
Q-1. What is the bandwidth of an amplifier?
Q-2. What are the upper and lower frequency limits of an amplifier?
Q-3. What are the upper and
lower frequency limits and the bandwidth for the amplifiers that have frequency-response curves as shown in figure
Figure 2-3A.—Frequency-response curves for Q3.
Figure 2-3B.—Frequency-response curves for Q3.
FACTORS AFFECTING FREQUENCY RESPONSE OF AN AMPLIFIER
In chapter 1 of this
module, the fact was mentioned that an audio amplifier is limited in its frequency response. Now you will see why
this is true.
You should recall that the frequency response of an a.c. circuit is limited by the reactive
elements (capacitance and inductance) in the circuit. As you know, this is caused by the fact that the capacitive
and inductive reactances vary with the frequency. In other words, the value of the reactance is determined, in
part, by frequency. Remember the formulas:
If you ignore the amplifying device (transistor, electron tube, etc.), and if the amplifier circuit is
made up of resistors only, there should be no limits to the frequency response. In other words, a totally
resistive circuit would have no frequency limits. However, there is no such thing as a totally resistive circuit
because circuit components almost always have some reactance. In addition to the reactance of other components in
the circuit, most amplifiers use RC coupling. This means that a capacitor is used to couple the signal in to and
out of the circuit. There is also a certain amount of capacitance and inductance in the wiring of the circuit. The
end result is that all circuits are reactive. To illustrate this point, figure 2-4 shows amplifier circuits with
the capacitance and inductance of the wiring represented as "phantom" capacitors and inductors. The reactances of
the capacitors (XC) and the inductors (XL) are shown as "phantom" variable resistors. View (A) shows the circuit
with a low-frequency input signal, and view (B) shows the circuit with a high-frequency input signal.
Figure 2-4A.—Amplifiers showing reactive elements and reactance.
Figure 2-4B.—Amplifiers showing reactive elements and reactance.
The actual circuit components are: C1, C2, C3, R1, R2, R3, and Q1. C1 is used to couple the input
signal. R1 develops the input signal. R2, the emitter resistor, is used for proper biasing and temperature
stability. C2 is a decoupling capacitor for R2. R3 develops the output signal. C3 couples the output signal to the
next stage. Q1 is the amplifying device.
The phantom circuit elements representing the capacitance and
inductance of the wiring are: L1, L2, C4, and C5. L1 represents the inductance of the input wiring. L2 represents
the inductance of the output wiring. C4 represents the capacitance of the input wiring. C5 represents the
capacitance of the output wiring.
In view (A) the circuit is shown with a low-frequency input signal.
Since the formulas for capacitive reactance and inductive reactance are:
You should remember that if frequency is low, capacitive reactance will be high and inductive reactance
will be low. This is shown by the position of the variable resistors that represent the reactances. Notice that
XL1 and XL2 are low; therefore, they do not "drop" very much of the input and output signals. XC4 and XC5 are
high; these reactances tend to "block" the input and output signals and keep them from going to the power supplies
(VBB and VCC). Notice that the output signal is larger in amplitude than the input signal.
Now look at view (B). The input signal is a high-frequency signal. Now XC is low and XL is high. XL1 and XL2
now drop part of the input and output signals. At the same time XC4 and XC5 tend to "short" or "pass" the input
and output signals to signal ground. The net effect is that both the input and output signals are reduced. Notice
that the output signal is smaller in amplitude than the input signal.
Now you can see how the capacitance
and inductance of the wiring affect an amplifier, causing the output of an amplifier to be less for high-frequency
signals than for low-frequency signals.
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