When analyzing a DC BJT circuit, the BJT is replaced by one of the DC circuit models shown below. (IE- 0) For CE Trans., IC = βIb + (1+β) Ico where β═α, 1- α is CE Gain Bulk-recombination current ICO Inc Ipe Ine Figure: An npn transistor with variable biasing sources (common-emitter configuration).Ĭommon-Emitter Circuit Diagram Collector-Current Curves VCE IC IC + _ Active Region VCC IB IB VCE Saturation Region Cutoff Region IB = 0īJT’s have three regions of operation: 1) Active - BJT acts like an amplifier (most common use) 2) Saturation - BJT acts like a short circuit 3) Cutoff - BJT acts like an open circuit BJT is used as a switch by switching between these two regions. + Holes B - + - + - p + + IB - VBE - _ įor CB Transistor IE= Ine+ Ipe Ic= Inc- Ico And Ic= - αIE + ICo CB Current Gain, α ═ (Ic- Ico).Carrier transport in the active base region directly beneath the heavily doped (n+) emitter dominates i-v characteristics of BJT. A small current also enters base terminal, crosses base-emitter junction and exits through emitter. Majority of current enters collector, crosses base region and exits through emitter.Consists of 3 alternate layers of n- and p-type semiconductor called emitter (E), base (B) and collector (C).Base current consists of holes crossing from the base into the emitter and of holes that recombine with electrons in the base. NOTE: Most of the current is due to electrons moving from the emitter through base to the collector. N I co - Inc + VCB - p- Electrons + Holes + Ipe Ine n+ VBE - Bulk-recombination Current Figure : Current flow (components) for an n-p-n BJT in the active region.
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