BJT as Amplifiers, Lecture notes of Analog Electronics

A detailed analysis of the use of bipolar junction transistors (bjts) as amplifiers. It covers various biasing techniques, including resistive divider biasing, accounting for base current, and pnp biasing. The document then delves into the study of the common-emitter (ce) topology, analyzing the ce core, including the early effect, and emitter degeneration. It also discusses the input and output impedances of the ce stage, as well as the tradeoffs between voltage gain and headroom. The document further explores the inclusion of the early effect and the impact of emitter degeneration on the ce stage. Additionally, it covers the common-base (cb) amplifier, comparing it to the ce stage, and examines the emitter follower topology. A comprehensive understanding of bjt amplifier design and analysis.

Typology: Lecture notes

2021/2022

Uploaded on 06/07/2022

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ANALOGUE ELECTRONICS
AENG001-4-2
CHAPTER 5
BJT as Amplifiers
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ANALOGUE ELECTRONICS

AENG001- 4 - 2

CHAPTER 5

BJT as Amplifiers

Chapter 5 BJT as Amplifiers

 5.1 General Considerations  5.2 Operating Point Analysis and Design  5.3 Bipolar Amplifier Topologies  5.4 Summary and Additional Examples

Voltage Amplifier

 In an ideal voltage amplifier, the input impedance is infinite and the output impedance zero.  But in reality, input or output impedances depart from their ideal values.

Input/Output Impedances

 The figure above shows the techniques of measuring input and output impedances. x x x i V R

Impedance at a Node

 When calculating I/O impedances at a port, we usually ground one terminal while applying the test source to the other terminal of interest.

Impedance at Collector

 With Early effect, the impedance seen at the collector is equal to the intrinsic output impedance of the transistor (if emitter is grounded). out o Rr

Three Master Rules of Transistor Impedances

 Rule # 1: looking into the base, the impedance is r if emitter is (ac) grounded.  Rule # 2: looking into the collector, the impedance is ro if emitter is (ac) grounded.  Rule # 3: looking into the emitter, the impedance is 1/gm if base is (ac) grounded and Early effect is neglected.

Biasing of BJT

 Transistors and circuits must be biased because (1) transistors must operate in the active region, (2) their small- signal parameters depend on the bias conditions.

Notation Simplification

 Hereafter, the battery that supplies power to the circuit is replaced by a horizontal bar labeled Vcc, and input signal is simplified as one node called Vin.

Example of Bad Biasing

 The microphone is connected to the amplifier in an attempt to amplify the small output signal of the microphone.  Unfortunately, there’s no DC bias current running thru the transistor to set the transconductance.

Biasing with Base Resistor

 Assuming a constant value for VBE, one can solve for both IB and IC and determine the terminal voltages of the transistor.  However, bias point is sensitive to  variations. B CC BE C B CC BE B R V V I R V V I     , 

Improved Biasing: Resistive Divider

 Using resistor divider to set VBE, it is possible to produce an IC that is relatively independent of  if base current is small. exp( ) 1 2 2 1 2 2 T CC C S X CC V V R R R I I V R R R V    

Emitter Degeneration Biasing

 The presence of RE helps to absorb the error in VX so VBE stays relatively constant.  This bias technique is less sensitive to  (I 1 >> IB) and VBE variations.

Design Procedure

 Choose an IC to provide the necessary small signal parameters, gm, r, etc.  Considering the variations of R 1 , R 2 , and VBE, choose a value for VRE.  With VRE chosen, and VBE calculated, Vx can be determined.  Select R 1 and R 2 to provide Vx.