Module 8—Introduction to Amplifiers
Pages i - ix
1-1 to 1-10
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2-21 to 2-30
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happens when you select a
channel on your television set or tune to a station on your radio. To accomplish this "tuning," you need only
change the value of inductance or capacitance in the parallel LC circuits (tuned circuits).
In most cases,
the capacitance is changed by the use of variable capacitors. The capacitors in the input and output portions of
all the RF amplifier stages are ganged together in order that they can all be changed at one time with a single
device, such as the tuning dial on a radio. (This technique will be shown on a schematic a little later in this
Q-20. If the input-signal-developing impedance of an amplifier is increased, what is the effect on the
Q-21. If the output impedance of an amplifier circuit is decreased, what is the effect on the
Q-22. What is the purpose of a frequency-determining network in an RF amplifier?
Q-23. Can a parallel LC circuit be used as the frequency-determining network for an RF amplifier?
Q-24. How can the frequency be changed in the frequency-determining network?
RF AMPLIFIER COUPLING
Figure 2-14 and the other circuits you have been shown use
capacitors to couple the signal in to and out of the circuit (C1 and C4 in figure 2-14). As you remember from
chapter 1, there are also other methods of coupling signals from one stage to another. Transformer coupling is the
most common method used to couple RF amplifiers. Transformer coupling has many advantages over RC coupling for rf
amplifiers; for example, transformer coupling uses fewer components than capacitive coupling. It can also provide
a means of increasing the gain of the stage by using a step-up transformer for voltage gain. If a
is required, a step-down transformer can be used.
You should also remember that the primary and secondary
windings of a transformer are inductors. With these factors in mind, an RF amplifier could be constructed like the
one shown in figure 2-15.
Figure 2-15.—Transformer-coupled RF amplifier.
In this circuit, the secondary of T1 and capacitor C1 form a tuned circuit which is the input-signal-
developing impedance. The primary of T2 and capacitor C2 are a tuned circuit which acts as the output impedance of
Q1. (Both T1 and T2 must be RF transformers in order to operate at RF frequencies.)
The input signal
applied to the primary of T1 could come from the previous stage or from some input device, such as a receiving
antenna. In either case, the input device would have a capacitor connected
across a coil to form a tuned circuit. In the same way, the secondary of T2 represents the output of
this circuit. A capacitor connected across the secondary of T2 would form a parallel LC network. This network
could act as the input-signal-developing impedance for the next stage, or the network could represent some type of
output device, such as a transmitting antenna.
The tuned circuits formed by the transformer and capacitors
may not have the bandwidth required for the amplifier. In other words, the bandwidth of the tuned circuit may be
too "narrow" for the requirements of the amplifier. (For example, the RF amplifiers used in television receivers
usually require a bandwidth of 6 MHz.)
One way of "broadening" the bandpass of a tuned circuit is to use a
swamping resistor. This is similar to the use of the swamping resistor that was shown with the series peaking coil
in a video amplifier. A swamping resistor connected in parallel with the tuned circuit will cause a much broader
bandpass. (This technique and the theory behind it are discussed in more detail in NEETS, Module 9.)
Another technique used to broaden the bandpass involves the amount of coupling in the transformers. For
transformers, the term "coupling" refers to the amount of energy transferred from the primary to the secondary of
the transformer. This depends upon the number of flux lines from the primary that intersect, or cut, the
secondary. When more flux lines cut the secondary, more energy is transferred.
Coupling is mainly a
function of the space between the primary and secondary windings. A transformer can be loosely coupled (having
little transfer of energy), optimumly coupled (just the right amount of energy transferred), or overcoupled (to
the point that the flux lines of primary and secondary windings interfere with each other).
(view A) (view B) (view C), shows the effect of coupling on frequency response when parallel LC circuits are made
from the primary and secondary windings of transformers.
Figure 2-16A.—Effect of coupling on frequency response. LOOSE COUPLING
Figure 2-16B.—Effect of coupling on frequency response. OPTIMUM COUPLING
Figure 2-16C.—Effect of coupling on frequency response. OVER-COUPLING
In view (A) the transformer is loosely coupled; the frequency response curve shows a narrow bandwidth.
In view (B) the transformer has optimum coupling; the bandwidth is wider and the curve is relatively flat. In view
(C) the transformer is overcoupled; the frequency response curve shows a broad bandpass, but the curve "dips" in
the middle showing that these frequencies are not developed as well as others in the bandwidth.
coupling will usually provide the necessary bandpass for the frequency-determining network (and therefore the RF
amplifier). For some uses, such as RF amplifiers in a television receiver, the bandpass available from optimum
coupling is not wide enough. In these cases, a swamping resistor (as mentioned earlier) will be used with the
optimum coupling to broaden the bandpass.
COMPENSATION OF RF AMPLIFIERS
have been shown the way in which an RF amplifier is configured to amplify a band of frequencies and the way in
which an RF amplifier can be "tuned" for a particular band of frequencies. You have also seen some ways in which
the bandpass of an RF amplifier can be adjusted. However, the frequencies at which RF amplifiers operate are so
high that certain problems exist.
One of these problems is the losses that can occur in a transformer at
these high frequencies. Another problem is with interelectrode capacitance in the transistor. The process of
overcoming these problems is known as COMPENSATION.
Transformers in RF Amplifiers
As you recall from NEETS, Module 1, the losses in a transformer are classified as copper loss, eddy-current loss,
and hysteresis loss. Copper loss is not affected by frequency, as it depends upon the resistance of the winding
and the current through the winding. Similarly, eddy-current loss is mostly a function of induced voltage rather
than the frequency of that voltage. Hysteresis loss, however, increases as frequency increases.
loss is caused by the realignment of the magnetic domains in the core of the transformer each time the polarity of
the magnetic field changes. As the frequency of the a.c. increases, the number of shifts in the magnetic field
also increases (two shifts for each cycle of a.c.); therefore, the "molecular friction" increases and the
hysteresis loss is greater. This increase in hysteresis loss causes the efficiency of the transformer (and
therefore the amplifier) to decrease. The energy that goes into hysteresis loss is taken away from energy that
could go into the signal.
RF TRANSFORMERS, specially designed for use with RF, are used to correct the
problem of excessive hysteresis loss in the transformer of an RF amplifier. The windings of RF transformers are
wound onto a tube of nonmagnetic material and the core is either powdered iron or air. These types of cores also
Neutralization of RF Amplifiers
The problem of interelectrode capacitance in the
transistor of an RF amplifier is solved by NEUTRALIZATION. Neutralization is the process of counteracting or
"neutralizing" the effects of interelectrode capacitance.
Figure 2-17 shows the effect of the
base-to-collector interelectrode capacitance in an RF amplifier. The "phantom" capacitor (CBC) represents the
interelectrode capacitance between the base and the collector of Q1. This is the interelectrode capacitance that
has the most effect in an RF amplifier. As you can see, CBC causes a degenerative (negative) feedback which
decreases the gain of the amplifier. (There are some special cases in which CBC can cause regenerative (positive)
feedback. In this case, the technique described below will provide negative feedback which will accomplish the
neutralization of the amplifier.)
Figure 2-17.—Interelectrode capacitance in an RF amplifier.
As you may recall, unwanted degenerative feedback can be counteracted (neutralized) by using positive
feedback. This is exactly what is done to neutralize an RF amplifier.
Positive feedback is accomplished by
the use of a feedback capacitor. This capacitor must feed back a signal that is in phase with the signal on the
base of Q1. One method of doing this is shown in figure
Figure 2-18.—Neutralized RF amplifier.
In figure 2-18, a feedback capacitor (C4) has been added to neutralize the amplifier. This solves the
problem of unwanted degenerative feedback. Except for capacitor C4, this circuit is identical to the circuit shown
in figure 2-17. (When CBC causes regenerative feedback, C4 will still neutralize the amplifier. This is true
because C4 always provides a feedback signal which is 180 degrees out of phase with the feedback signal caused by
Q-25. What is the most common form of coupling for an RF amplifier?
Q-26. What are two
advantages of this type of coupling?
Q-27. If current gain is required from an RF amplifier, what type
of component should be used as an output coupling element?
Q-28. What problem is caused in an RF
amplifier by a loosely coupled transformer? Q-29. How is this problem corrected?
Q-30. What problem is caused by overcoupling in a transformer?
Q-31. What method provides the widest
Q-32. What two methods are used to compensate for the problems that cause low gain in an RF
Q-33. What type of feedback is usually caused by the base-to-collector interelectrode
Q-34. How is this compensated for?
TYPICAL RF AMPLIFIER CIRCUITS
As a technician, you will see many different RF amplifiers in many different pieces of equipment. The
particular circuit configuration used for an RF amplifier will depend upon how that amplifier is used. In the
final part of this chapter, you will be shown some typical RF amplifier circuits.
Figure 2-19 is the schematic diagram of a typical RF amplifier that is used in an AM radio receiver.
In figure 2-19, the input circuit is the antenna of the radio (L1-a coil) which forms part of an LC circuit which
is tuned to the desired station by variable capacitor C1. L1 is wound on the same core as L2, which couples the
input signal through C2 to the transistor (Q1). R1 is used to provide proper bias to Q1 from the base power supply
(VBB). R2 provides proper bias to the emitter of Q1, and C3 is used to bypass R2. The primary of T1 and capacitor
C4 form a parallel LC circuit which acts as the load for Q1. This LC circuit is tuned by C4, which is ganged to C1
allowing the antenna and the LC circuit to be tuned together. The primary of T1 is center-tapped to provide proper
impedance matching with Q1.
Figure 2-19.—Typical AM radio RF amplifier.
You may notice that no neutralization is shown in this circuit. This circuit is designed for the AM
broadcast band (535 kHz - 1605 kHz).
At these relatively low RF frequencies the degenerative feedback
caused by base-to-collector interelectrode capacitance is minor and, therefore, the amplifier does not need
Figure 2-20 is a typical RF amplifier used in a vhf television receiver. The input-signal-developing circuit for
this amplifier is made up of L1, C1, and C2. The inductor tunes the input-signal-developing circuit for the proper
TV channel. (L1 can be switched out of the circuit and another inductor switched in to the circuit by the channel
selector.) R1 provides proper bias to Q1 from the base supply voltage (VBB). Q1 is the transistor. Notice that the
case of Q1 (the dotted circle around the transistor symbol) is shown to be grounded. The case must be grounded
because of the high frequencies (54 MHz - 217 MHz) used by the circuit. R2 provides proper bias from the emitter
of Q1, and C3 is used to bypass R2. C5 and L2 are a parallel LC circuit which acts as the load for Q1. The LC
circuit is tuned by L2 which is switched in to and out of the LC circuit by the channel selector. L3 and C6 are a
parallel LC circuit which develops the signal for the next stage. The parallel LC circuit is tuned by L3 which is
switched in to and out of the LC circuit by the channel selector along with L1 and L2. (L1, L2, and L3 are
actually part of a bank of inductors. L1, L2, and L3 are in the circuit when the channel selector is on channel 2.
For other channels, another group of three inductors would be used in the circuit.) R3 develops a signal which is
fed through C4 to provide neutralization. This counteracts the effects of the interelectrode capacitance from the
base to the collector of Q1. C7 is used to isolate the RF signal from the collector power supply (VCC).
Figure 2-20.—Typical VHF television RF amplifier.
The following questions refer to figure 2-21.
Figure 2-21.—Typical RF amplifier.
Q-35. What components form the input-signal-developing impedance for the amplifier?
Q-36. What is the purpose of R1?
Q-37. What is the purpose of R2?
Q-38. If C4 were removed from the circuit, what would
happen to the output of the amplifier?
Q-39. What components form the load for Q1?
How many tuned parallel LC circuits are shown in this schematic?
Q-41. What do the dotted lines connecting C1, C2, C5, and C6 indicate?
Q-42. What is the purpose of C3?
This chapter has presented
information on video and RF amplifiers. The information that follows summarizes the important points of this
A FREQUENCY-RESPONSE CURVE will enable you to determine the BANDWIDTH and the
UPPER and LOWER FREQUENCY LIMITS of an amplifier.
The BANDWIDTH of an amplifier is determined by the formula:
The UPPER-FREQUENCY RESPONSE of an amplifier is limited by the inductance and
capacitance of the circuit.
The INTERELECTRODE CAPACITANCE of a transistor causes DEGENERATIVE FEEDBACK at high
VIDEO AMPLIFIERS must have a frequency response of 10 hertz to 6 megahertz (10 Hz - 6 MHz).
To provide this frequency response, both high- and low-frequency compensation must be used.
PEAKING COILS are used in video amplifiers to overcome the high-frequency limitations caused by the
capacitance of the circuit.
SERIES PEAKING is accomplished by a peaking coil in series with the output-signal
SHUNT PEAKING is accomplished by a peaking coil in parallel (shunt) with the
Introduction to Matter, Energy, and Direct Current,
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Introduction to Amplifiers, Introduction to
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