Common Emitter configuration of transistor, characteristics, application
Friends, today we
will read about the common emitter configuration of BJT
transistor. In this lecture, we will know its diagram, its characteristics and
its application. We call it common emitter, because the
emitter terminal is the common terminal between input and
output. In this configuration, the base is input and the collector is output.
Application:-
Properties: -
1) The input impedance is the ratio of change in base emitter voltage (VBE) to change in base current when collector emitter voltage (VCE) is constant.
Ri
= (ΔVBE / ΔIB)VCE
2)
Ro =
3) Its voltage gain is high.
4) Its current gain is high.
5) Its power gain is high.
5) It also has a current amplification factor, which we call β. β is known as the ratio of change in output current to change in input current.
β = ΔIC / ΔIB
Construction Diagram:-
As you know very well that for amplification we use transistor in active region. So we will understand the diagram of NPN and PNP transistor in active region very well. As shown in the diagram, the base terminal of transistor is connected to the one side of base resistance (RB). Other side of base resistance (RB) is connected to the positive terminal of VBB.
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CE configuration of NPN |
Negative terminal of VBB is directly connected to the ground terminal. Emitter of transistor is also connected to the ground terminal. Collector of transistor is connected to the one side of collector resistance (RC). Other side of collector resistance (RC) is connected to the positive terminal of VCC. Negative terminal of VCC is directly connected to the ground terminal.
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CE configuration of PNP |
Working:-
The base emitter of the transistor is forward bias junction which we call VBE. And its collector emitter of the transistor is reverse bias junction which we call VCE.
Expression:-
We had two equations in common base configuration.
IE = IB + IC ------------- (i)
IC = α.IE + ICBO -------- (ii)
Put the value of IE from equation (i) in equation (ii)
IC = α.(IB + IC) + ICBO
IC = α.IB + α.IC + ICBO
IC - α.IC = α.IB + ICBO
IC(1 - α) = α.IB + ICBO
Dividing both side by (1 - α).
IC(1 - α) / (1 - α) = α.IB / (1 - α) + ICBO / (1 - α)
IC = α.IB / (1 - α) + ICBO / (1 - α) --------- (iii)
We know that
α = β / 1+β
Put the value of α in equation (iii)
IC = β / 1+β .IB / (1 - β / 1+β ) + ICBO / (1 - β / 1+β)
IC = β / 1+β .IB / (1 - β + β / 1+β ) + ICBO / (1 - β + β / 1+β)
IC = β / 1+β .IB / (1 / 1+β ) + ICBO / (1 / 1+β)
IC = β / 1+β . (1+β / 1). IB + ICBO .1+β / 1
IC = β. IB + ICBO .(1+β)
We know that what is ICBO. It is the leakage current for common base configuration. But in case of common emitter configuration, the leakage current is the combination of ICBO .(1+β). We can say that
ICBO .(1+β) = ICEO
ICEO is the leakage current of common emitter configuration. It is the current between collector and emitter terminal when base terminal of the transistor is open ie IB =0, So
IC = β. IB + ICEO
This leakage current ICEO we can neglect because it much smaller than IB
So IC = β. IB
β = IC / IB
:- β = Current amplification factor for common emitter
The value of β is lies between 20 to 500.
Input characteristics of common emitter configuration:-
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Input characteristics of CE configuration |
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Input characteristics Chart of CE configuration |
Output characteristics of common emitter configuration:-
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Output characteristics of CE configuration |
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Output characteristics chart of CE configuration |
Waveform:-
Its input waveform has a low signal and in its output waveform we get a high signal. But its input and output waveform invert each other.
Click to know about Common Base configuration
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