Small Signal Model PNP Transistor Section 4.1-4.4,4.6.

Slides:



Advertisements
Similar presentations
Differential Amplifiers and Integrated Circuit (IC) Amplifiers
Advertisements

Common-Collector Amplifier Section Topics Emitter Follower as a power amplifier Push and Pull Output Stage.
Common Emitter Amplifier. Design Rules V RE should be > 100 mV.
Transistors and transistor circuits
BIJUNCTION TRANSISTOR
Cascode Stage. OUTLINE Review of BJT Amplifiers Cascode Stage Reading: Chapter 9.1.
Physics of Bipolar Junction Transistor Section
Chapter 4 Bipolar Junction Transistor
EE105 Fall 2007Lecture 6, Slide 1Prof. Liu, UC Berkeley Lecture 6 OUTLINE BJT (cont’d) – PNP transistor (structure, operation, models) BJT Amplifiers –
EE105 Fall 2007Lecture 5, Slide 1Prof. Liu, UC Berkeley Lecture 5 OUTLINE BJT (cont’d) – Transconductance – Small-signal model – The Early effect – BJT.
Department of EECS University of California, Berkeley EECS 105 Fall 2003, Lecture 14 Lecture 14: Bipolar Junction Transistors Prof. Niknejad.
Lecture 7 ANNOUNCEMENTS OUTLINE BJT Amplifiers (cont’d)
BJT in Saturation Mode Section 4.5.
Part B-3 AMPLIFIERS: Small signal low frequency transistor amplifier circuits: h-parameter representation of a transistor, Analysis of single stage transistor.
Small Signal Model PNP Transistor Section 4.4. BJT in the active region Electrons cross the forward biased BE junction and are swept reverse biased BC.
BJT (cont’d). OUTLINE – Transconductance – Small-signal model – The Early effect – BJT operation in saturation mode Reading: Chapter
1 Tai-Cheng Lee Spring 2006 Bipolar Junction Transistors (BJT) Tai-Cheng Lee Electrical Engineering/GIEE, NTU.
Problems on Terminal Resistances Chapter 5. Schedule 153/4TuesdayTerminal Resistance (R B, R C and R E ) L3/4Tuesday small signal model from Cadence,
Introduction to BJT Amplifier BJT (Review). Still remember about BJT? The emitter current (i E ) is the sum of the collector current (i C ) and the base.
Chapter 4 Bipolar Junction Transistors
BJT Amplifier. BJT Amplifiers: Overview Voltage Amplifier In an ideal voltage amplifier, the input impedance is infinite and the output impedance is.
Transistor Amplifier Basics It is critical to understand the notation used for voltages and currents in the following discussion of transistor amplifiers.
The Bipolar Junction Transistor
EENG 3520: Electronics II Lecture 3 Oluwayomi Adamo.
PNP Section 4.3,3.6. Schedule 109/25ThursdayPNP 4.3, /30TuesdayBJT in saturation 4.5 L9/30Tuesday Measure Beta of a transistor.
BJT transistors Summary of DC problem 2 Bias transistors so that they operate in the linear region B-E junction forward biased, C-E junction reversed.
Chapter 13 Small-Signal Modeling and Linear Amplification
Chapter 4 Bipolar junction transistor Ir. Dr. Rosemizi Abd Rahim 1 Ref: Electronic Devices and Circuit Theory, 10/e, Robert L. Boylestad and Louis Nashelsky.
Chapter 13 Small-Signal Modeling and Linear Amplification
CHAPTER 10 AC Power Bipolar Junction Transistors: Operation, Circuit Models, and Applications.
LECTURE 1: BASIC BJT AMPLIFIER -AC ANALYSIS-
CHAPTER 2 Forward Biased, DC Analysis AC Analysis Reverse Biased
Recall Last Lecture Biasing of BJT Three types of biasing
Bipolar Junction Transistor Circuit Analysis
Electronics The Eleventh and Twelfth Lectures
EKT104 ANALOG ELECTRONIC CIRCUITS [LITAR ELEKTRONIK ANALOG] BASIC BJT AMPLIFIER (PART I) DR NIK ADILAH HANIN BINTI ZAHRI
Dept. of ECE, Univ. of Houston
Lecture 4 Bipolar Junction Transistors (BJTs)
Transistor Amplifier Basics
Bipolar Junction Transistors (BJT)
Lecture 10 Bipolar Junction Transistor (BJT)
Common Emitter Characteristics
Open book, open notes, bring a calculator
Chapter 4 Bipolar Junction Transistor
TRANSISTOR.
ENEE 303 1st Discussion.
Bipolar Junction Transistor
Electronics The Eleventh and Twelfth Lectures
SMALL SIGNAL ANALYSIS OF CB AMPLIFIER
SMALL SIGNAL ANALYSIS OF CE AMPLIFIER
Small-Signal Modeling and Linear Amplification
Chapter 1 – Revision Part 2
ترانزیستور BJT دکتر سعید شیری فصل پنجم از:
Electronics Fundamentals
Lecture’s content Objectives BJT – Small Signal Amplifier
Lecture 26 OUTLINE The BJT (cont’d) Ideal transistor analysis
Bipolar Junction Transistor Circuit Analysis
Lecture 25 OUTLINE The BJT (cont’d) Ideal transistor analysis
Lecture 25 OUTLINE The BJT (cont’d) Ideal transistor analysis
Common Emitter Amplifier
Lecture 26 OUTLINE The BJT (cont’d) Ideal transistor analysis
Introduction to Small Signal Model
Lecture 11 ANNOUNCEMENTS OUTLINE Review of BJT Amplifiers
Chapter 4 Bipolar Junction Transistor
Transistor A simplified structure of the npn transistor.
Small Signal Model Section 4.4.
ChapTer FoUr DC BIASING - BIPOLAR JUNCTION TRANSISTORS (BJTs)
Review & Problems.
Bipolar Junction Transistors
Chapter 13 Small-Signal Modeling and Linear Amplification
Presentation transcript:

Small Signal Model PNP Transistor Section ,4.6

Schedule 92/11TuesdayPhysics of a BJT L2/11TuesdayMeasure Beta of a transistor 102/13ThursdayPNP /18TuesdayBJT in saturation mode4.5 L2/18Tuesday BJT in saturation/BJT implementation of an NAND gate 122/20ThursdaySmall Signal model [homework: small eq. circuit, (PNP)] 4.4,4.6

Overview

Review

Small Signal Model Section 4.4

Schematic of an Audio Amplifier Microphone produces a small signal. How does the amplifier circuit respond to a small change in the input signal? How is the analysis performed? Small signal model

Small Signal Analysis (For a Circuit You have not Seen Before) 1.Replace each ideal DC voltage source with a small signal ground. 2.Replace each ideal DC current source with an open circuit. 3.Replace each transistor by its small signal model 4.Analyze the small signal equivalent circuit.

Small Signal Analysis (For a Circuit You have not Seen Before) 1.Analyze the Circuit by Inspection

Voltage Source DC Voltage Source in Small Signal Analysis R S should be 0 for a good battery!

Current Source R S should be infinity for a good battery!

Small Signal Model (NPN)(PNP) Statements that are always true for both NPN and PNP. 1.r π is between B and E. 2.the direction of the dependent current source always points from the collector to emitter. 3. r o is always between B and C.

Question Replace Q1 and Q2 by their small equivalent circuit.

Answer

Question

Answer

Derivation of the Small Signal Model

Change in the Collector Current Due to a Small Change in Base-Emitter Voltage If a signal changes the base-emitter voltage by a small amount, how much change is produced in the collector current ?

Derivation of Transconductance If a signal changes the base-emitter voltage by a small amount, how much change is produced in the collector current ? Small signal model of Q1

But there is something else…. A change in V BE creates a change in base current! Small signal model

Example 4.10 Signal Generated By a microphone Small Signal Equivalent Circuit V BE =800 mV β=100 I S,Q1 =3 x A Question: If a microphone generates a 1 mV signal, how much change is observed in the collector and base current ?

A Simple Amplifier Determine the output signal level if the microphone produces a 1 mV signal.

AC Ground The voltage produced by a voltage source is constant. The small signal model is concerned only with changes in quantities. Therefore, a DC voltage source must be replaced with a ground in small signal analysis.

Example Small Signal Model

Summary

Output Resistance Due to Early Effect A larger reverse bias voltage leads to a larger BC depletion region. The effective base width (WB) is reduced. The slope of the electron profile increases. I C increases as VCE is increased.

Early Effect

James M. Early

Modeling of Early Effect

What Doesn’t Change with Early Effect ?

Modification of the Small Signal Model

Slides to Cover During the Lab

A Simple Cadence Example

Assumption Assume that 1.The DC at Vout is 0.9 V 2.g m =1 mS Gain is approximately equal to –g m R C. Bias current is I C =g m V t R=(1.8V-0.9V)/26uA=34.6 Kohms Gain is

DC Bias of the Amplifier

Sweep the Base Voltage to Get the IC=26 uA

Display the Transconductance

Display Transconductance

Verify Transconductance (1)

Verify Transconductance (2)

Transconductance VBIC mV25.64 uA mV26.64 uA ∆VBE1 mV ∆IC1 uA gm=∆VBE/∆IC1 mS

Introduce a Small Signal

Calculate Peak to Peak Voltage

Peak to Peak Voltage=67.78 mV mV/2=33.9