TRANSISTOR CONFIGURATIONS
Common Emitter
The common-emitter
configuration (CE) shown in figure 2-16 view A is the arrangement most
frequently used in practical amplifier circuits, since it provides good
voltage, current, and power gain. The common emitter also has a somewhat low
input resistance (500 ohms-1500 ohms), because the input is applied to the
forward-biased junction, and a moderately high output resistance (30
kilohms-50 kilohms or more), because the output is taken off the
reverse-biased junction. Since the input signal is applied to the
base-emitter circuit and the output is taken from the collector-emitter
circuit, the emitter is the element common to both input and output.
Since you have already
covered what you now know to be a common-emitter amplifier (fig. 2-12),
let's take a few minutes and review its operation, using the PNP
common-emitter configuration shown in figure 2-16 view A.
When a transistor is
connected in a common-emitter configuration, the input signal is injected
between the base and emitter, which is a low resistance, low-current
circuit. As the input signal swings positive, it also causes the base to
swing positive with respect to the emitter. This action decreases forward
bias which reduces collector current (IC) and increases collector
voltage (making VC more negative). During the negative
alternation of the input signal, the base is driven more negative with
respect to the emitter. This increases forward bias and allows more current
carriers to be released from the emitter, which results in an increase in
collector current and a decrease in collector voltage (making VC
less negative or swing in a positive direction). The collector current that
flows through the high resistance reverse-biased junction also flows through
a high resistance load (not shown), resulting in a high level of
amplification.
Since the input signal to
the common emitter goes positive when the output goes negative, the two
signals (input and output) are 180 degrees out of phase. The common-emitter
circuit is the only configuration that provides a phase reversal.
The common-emitter is the
most popular of the three transistor configurations because it has the best
combination of current and voltage gain. The term GAIN is used to describe
the amplification capabilities of the amplifier. It is basically a ratio of
output versus input. Each transistor configuration gives a different value
of gain even though the same transistor is used. The transistor
configuration used is a matter of design consideration. However, as a
technician you will become interested in this output versus input ratio
(gain) to determine whether or not the transistor is working properly in the
circuit.
The current gain in the
common-emitter circuit is called BETA (). Beta is the relationship of
collector current (output current) to base current (input current). To
calculate beta, use the following formula:
![](trans7a_files/image001.gif)
( is the Greek letter
delta, it is used to indicate a small change)
For example, if the input
current (IB) in a common emitter changes from 75 A to 100 A and
the output current (IC) changes from 1.5 mA to 2.6 mA, the
current gain (I) will be 44.
![](trans7a_files/image002.gif)
This simply means that a
change in base current produces a change in collector current which is 44
times as large.
You may also see the term
hfe used in place of I. The terms hfe and Iare
equivalent and may be used interchangeably. This is because "hfe"
means: h = hybrid (meaning mixture)
f = forward current
transfer ratio
e = common emitter configuration
The resistance gain of
the common emitter can be found in a method similar to the one used for
finding beta:
![](trans7a_files/image003.gif)
Once the resistance gain
is known, the voltage gain is easy to calculate since it is equal to the
current gain (I) multiplied by the resistance gain (E = IR). And, the power
gain is equal to the voltage gain multiplied by the current gain I (P = IE).
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