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Bipolar Junction Transistor

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Master the fundamentals of the Bipolar Junction Transistor (BJT) for your electronics and semiconductor physics exams! This comprehensive guide breaks down this crucial component with clear explanations, diagrams, and practical examples. Key Topics Covered: · Structure & Operation: NPN vs. PNP transistors, and the concept of current control. · Operating Modes: Detailed analysis of Active, Saturation, and Cut-off regions. · Configurations: Characteristics of Common-Emitter, Common-Base, and Common-Collector circuits. · Biasing & Stabilization: Essential biasing circuits (e.g., Voltage Divider Bias) and their analysis. · Small-Signal Model: Understanding the hybrid-pi model and AC equivalent circuits for amplifier design. · Key Formulas: Current gain (β), input/output impedance, and voltage gain calculations. What You Get: · Concise, well-structured notes perfect for efficient revision. · Clear diagrams illustrating concepts and characteristics curves. · Essential insights for solving both theoretical and numerical problems. Stop stressing! This document is your ultimate resource to build a solid understanding of BJTs and achieve a top grade. Download now and conquer your exams

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Bipolar Junction (BJT) transistors

A bipolar junction transistor is formed by joining three sections of semiconductors with
different types of doping. The middle section (base) is narrow and one of the other two
regions (emitter) is heavily doped. Two variants of BJT are possible: NPN and PNP.




Fig. 1

A BJT has three terminals. Six parameters; iC, iB, iE, vB, vE and vC; define the state of the
transistor. However, because BJT has three terminals, KVL and KCL should hold for these
terminals, i.e.,




Fig. 2

Operation of NPN Transistor

For proper operation, the emitter-base junction is forward biased and the collector-base junction
is reverse biased as shown in Fig. 3 When the emitter-base junction is forward biased say 100
electrons are emitted into the base resulting in emitter terminal current IE. Say two electrons
recombine in the base resulting in a base terminal current IB Say 98 electrons find themselves in
the depletion region at the collector-base junction because the base is thin and lightly doped. This
means the transition time is little and very few electrons will recombine because there are few
holes in the base. The 98 electrons are quickly swept across the collector-base junction by the
exposed ions at the junction and reach the collector terminal. This constitutes collector current I C.
Thus IE = IB + IC

, Fig. 3

Operation of PNP Transistor

PNP transistor behaves exactly in the same way as the NPN transistor. The only
difference is that the majority charge carriers are holes and minority charge carriers are
electrons.




Fig. 4

Transistor Configurations:

Common Base (CB) configuration

The base terminal is common between input and output circuits.

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