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Abstract: This describes the D.C. parameters of BJT.

Analog Electronics Lecture 2_PartC_I-V output characteristics of BJT

Key words;BJT;

Abstract: This describes the D.C. parameters of BJT.

BJT Common Base Configuration :

For CB Configuration :

I C = α F MI E + I CBO

Where α F = D.C. Forward current transfer Ratio of CB BJT = I C /I E ;

M = Avalanche Multiplication Factor at Base-Collector Junction given by = 1/[1-(Vcb/BVcbo)^n]

Where n= Miller Indices =2~6

I CBO = Reverse leakage current at CB Jn with emitter open.

= Avalanche breakdown voltage at CB Jn with emitter open

OUTPUT CHARACTERISTICS OF Common Base Bipolar Junction transistor

I C = I CBO when I E = 0 mA. This is the reverse leakage current at CB Junction with Emitter open and is of nA range.

BJT Common Emitter(CE) Configuration:

For CE Configuration :

I C = α F MI E + I CBO

=>I C = α F M(I B +I C ) + I CBO

=>I C (1-α F M)= α F MI B + I CBO

If M=1,

Where α F =0.99.

At low voltages we have M=1.

Then we get:

That is:

OUTPUT CHARACTERISTICS OF Common Emitter Bipolar Junction transistor

NOTE:-The slope in the figure is due to base width modulation which is also known as Early Effect.

I C = I CEO when I B = 0 mA. This is the collector junction leakage current at CB Junction with Base open and is of µA range.

Let us consider :

If α F M =1, then

At this point , break over occurs. And we have BV CEO =Break-over Voltage with Base Circuit open.

When α F M =1

That is

But :

Thus :

Thus:

Putting the required Values i.e. BV CBO =30V, β F = 100 , we get V CB * =18 V = BVceo ;

Now we have to know more about BV CES (Breakover Voltage when the base circuit is shorted)

BV CBO >BV CEX >BV CES >BV CEO

Where BV CBO = Breakover Voltage of the collector base junction when the emitter circuit is open.

BV CEX = Breakover Voltage of CE BJT for a given termination R X at the base

BV CEO = Breakover Voltage of CE BJT when the base circuit is open.

BV CES = Breakover Voltage of CE BJT when the base circuit is shorted to ground.

BV CEX = Breakover Voltage when the base circuit is connected to ground through a source Resistance (R S ) .

By proper base termination, the permissible region of operation can be extended upto BV CBO .

Thus we have seen that breakover occurs at α F M =1. At low current α F is very small, almost about 0.1.Therefore voltage has to be taken to a large value to satisfy α F M =1. But as soon as breakover occurs large current starts flowing. With large current α F improves from 0.1 to 0.99. Hence α F M =1 is satisfied at lower voltage Vs. Therefore breakover curves settles down at Vs. This voltage V S is known as sustaining voltage. Because of the fact that :

V S <BV CEO

We get a S Type Negative Impedance Region(NIR). In SCR and UJT also we get S Type NIR but in Tunnel Diode as shown in the Figure below we get N Type NIR.

COMPARISON BETWEEN COMMON BASE AND COMMON EMITTER CONFIGURATIONS

S.No. COMMON BASE COMMON EMITTER
1 h rb (reverse transmission factor)~10 -5 Thus it behaves as a near unilateral device. h re ~10 -4 Thus it behaves as a non-unilateral device.
2 In RF applications the circuit has a high probability of parasitic oscillations but in CB because of near unilaterality , probability of parasitic oscillation goes down. Hence for RF applications CB is the preferred circuit configuration. At low frequencies there is no danger of parasitic oscillations hence CE can be used even with poor reverse transmission factor.
3 h ob = 1/(2M)Thus it behaves as a near ideal current source. Thus it is very suitable for charging a capacitance with a constant current to generate a saw-tooth waveform. h oe =1/(40K)Thus it behaves as a non-ideal current source.

Both CB and CE are Current Controlled Current Source. CB is a near ideal CCCS whereas CE is a non-ideal CCCS.

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Source:  OpenStax, Solid state physics and devices-the harbinger of third wave of civilization. OpenStax CNX. Sep 15, 2014 Download for free at http://legacy.cnx.org/content/col11170/1.89
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