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Imporatnt modes of transistor operation

              Junction bias condition

1.

2.

3.

Mode Emitter-base Collector-base
Forward-Active

Saturation

Cut-off

Forward

Forward

Reverse

Reverse

Forward

Reverse

Active region :

figure1 Base emitter junction                                               figure3       figure2 collector base junction

Junction BE is forward biased. Hence holes from P move towards N (Ipe) and electrons move from N to P side (Ine) .

Ie= Ipe + Ine

Ipe is made up of holes going from P to N and part of these combines with electrons in base and constittues current Ib= Ipe-Ipc1. Rest of holes cross to collector and constitute current Ipc1 (collector current).

Junction CB is reverse biased as in figure. So electrons move from P to N (Ipc0) and holes move from N to P (Inc0).

|Ic0| = Ipc0 + Inc0 ( mod because directions are opposite as per figure.)

Ico = Icbo (figure 1)

Ic = -αIe + Icbo ( apply KCL in figure).

Saturation region :

Veb = constant so that Ie = constant.

Ic = Ic’ – Ie

If Vcb is negative then CB junction is reverse biased so only small reverse saturation current flows. When Vcb increased from –ve to + ve CB becomes forward biased and large Ic starts flowing. Hence in saturation maximum collector current flows.

 


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