Chapter 6 4 min read
Save

Bipolar Junction Transistor

Fundamentals of Electrical and Electronics · BCA · Updated Apr 06, 2026

Table of Contents

Unit VI: Bipolar Junction Transistor (BJT)

Duration: 4 Hours | Credit: ELX 133.3

Introduction to Bipolar Junction Transistors

A Bipolar Junction Transistor (BJT) is a three-terminal semiconductor device that uses two junctions to achieve signal amplification and switching. It is one of the most important electronic components and forms the basis of many integrated circuits.

BJT Structure and Operation

Physical Structure

A BJT consists of three regions of semiconductors:

  • Emitter (E): Heavily doped region that supplies charge carriers
  • Base (B): Thin, lightly doped region that controls current flow
  • Collector (C): Moderately doped region that collects charge carriers

Two Types of BJTs

  • NPN Transistor: n-type emitter, p-type base, n-type collector
  • PNP Transistor: p-type emitter, n-type base, p-type collector

BJT Biasing Conditions

Forward-Active Region (Amplification Mode)

  • Base-Emitter junction is forward-biased (VBE > 0.6V for silicon)
  • Base-Collector junction is reverse-biased (VCB < -0.2V for silicon)
  • Emitter injects carriers into base
  • Collector collects carriers from base
  • Moderate collector current with small base current (amplification occurs)

Saturation Region

  • Both junctions are forward-biased
  • Maximum collector current (limited by external resistances)
  • Transistor acts as a closed switch (very low VCE, typically < 0.2V)

Cutoff Region

  • Base-Emitter junction is reverse-biased (VBE < 0)
  • Emitter-Base junction is off
  • Collector current is nearly zero (only leakage current)
  • Transistor acts as an open switch

BJT Current Relationships

Current Gain (β)

β = IC / IB (current gain)

  • Also called dc current gain or hFE
  • Typical values: 50-300 for small-signal transistors
  • Varies with collector current and temperature
  • More stable at moderate current levels

Emitter Current

IE = IC + IB

IC = β × IB

IE = (1 + β) × IB = α × IC / (1 - α)

Transport Factor (α)

α = IC / IE (typically 0.98-0.9999)

β = α / (1 - α)

Ebers-Moll Model

Transistor as Two Diodes

The Ebers-Moll model represents a transistor as two diodes with common current source:

  • Base-Emitter diode (forward-biased in normal operation)
  • Base-Collector diode (reverse-biased in normal operation)
  • Controlled current source representing amplification

Hybrid-π Model

Used for small-signal AC analysis with parameters like:

  • re: Emitter resistance
  • rb: Base resistance
  • rμ: Collector resistance
  • gm: Transconductance (mutual conductance)

BJT Configurations

Common Emitter Configuration

  • Input: Base terminal
  • Output: Collector terminal
  • Common: Emitter terminal
  • Voltage Gain: Moderate to high (50-500)
  • Current Gain: β (50-300)
  • Input Impedance: Moderate (1-10 kΩ)
  • Output Impedance: Moderate to high (10-100 kΩ)
  • Application: General-purpose amplifier

Common Collector Configuration (Emitter Follower)

  • Input: Base terminal
  • Output: Emitter terminal
  • Common: Collector terminal
  • Voltage Gain: Less than 1 (unity gain)
  • Current Gain: β (large, 50-300)
  • Input Impedance: Very high (100 kΩ - 1 MΩ)
  • Output Impedance: Very low (10-100 Ω)
  • Application: Buffer, impedance matching

Common Base Configuration

  • Input: Emitter terminal
  • Output: Collector terminal
  • Common: Base terminal
  • Voltage Gain: Moderate to high (100-1000)
  • Current Gain: α (close to 1, 0.98-0.9999)
  • Input Impedance: Very low (20-100 Ω)
  • Output Impedance: Very high (100 kΩ - 1 MΩ)
  • Application: High-frequency amplifier

BJT Biasing and DC Operating Point

Biasing Objectives

  1. Establish a stable Q-point (operating point) independent of β variations
  2. Ensure adequate bias current to maintain linear operation
  3. Maximize available output voltage swing

Fixed-Base Bias

Simple but unstable because IB depends directly on β which varies with temperature and manufacturing

Voltage Divider Bias (Stiff Bias)

Most practical method:

  • Uses a voltage divider to establish base voltage
  • Base voltage is relatively independent of β
  • More stable with temperature changes

Load Line and Q-Point

DC Load Line Equation

IC = (VCC - VCE) / RC

Q-Point (Quiescent Point)

The intersection of the dc load line with the transistor characteristic curve determines the operating point (Q-point) with coordinates (VCE,Q, IC,Q)

Graphical Solution

  • Plot the DC load line from (VCC, 0) to (0, VCC/RC)
  • Plot the IB line from the specified base current
  • Find intersection of IB curve with load line to find Q-point

Temperature Effects and Stability

Temperature Sensitivity

  • β increases with temperature (0.5%/°C)
  • VBE decreases with temperature (2 mV/°C)
  • ICO (leakage current) doubles for every 25-50°C

Thermal Runaway

Risk of instability where increased temperature leads to increased current, causing more heat generation

Key Takeaways

  • BJT has three terminals: Emitter, Base, and Collector
  • Current gain β = IC / IB
  • Forward-active region provides amplification
  • Saturation and cutoff regions are used for switching
  • Common Emitter provides moderate voltage and current gain
  • Common Collector (Emitter Follower) provides high input impedance
  • Common Base provides high frequency response
  • Proper biasing ensures stable operation over temperature range

Related Notes

Discussion

0 comments

Join the discussion

Log in to share your thoughts and help fellow students.

Log in to comment

No comments yet. Be the first to share your thoughts!