S. RossEECS 40 Spring 2003 Lecture 14 Last time… I V +_+_ Reverse breakdown Reverse bias Forward bias I V ZK VFVF V Focus we introduced the diode and its.

Slides:



Advertisements
Similar presentations
Lecture 6 Solid-State Diodes and Diode Circuits
Advertisements

Lecture 4: Signal Conditioning
Diodes and diode equation
EE462L, Spring 2014 DC−DC Boost Converter
Fundamentals of Microelectronics
Announcements Assignment 2 due now Assignment 3 posted, due Thursday Oct 6 th First mid-term Thursday October 27 th.
S. RossEECS 40 Spring 2003 Lecture 21 CMOS INVERTER CMOS means Complementary MOS: NMOS and PMOS working together in a circuit D S V DD (Logic 1) D S V.
Review of Circuit Analysis
S. RossEECS 40 Spring 2003 Lecture 27 Today we will Put a twist on our normally linear operational amplifier circuits to make them perform nonlinear computations.
S. RossEECS 40 Spring 2003 Lecture 13 SEMICONDUCTORS: CHEMICAL STRUCTURE Start with a silicon substrate. Silicon has 4 valence electrons, and therefore.
Lecture 15, Slide 1EECS40, Fall 2004Prof. White Lecture #15 OUTLINE The pn Junction Diode -- Uses: Rectification, parts of transistors, light-emitting.
10/15/2004EE 42 fall 2004 lecture 201 Lecture #20 Review Reminder: MIDTERM coming up next week (Monday October 18 th ) This week: Review and examples.
S. RossEECS 40 Spring 2003 Lecture 20 Today we will Review NMOS and PMOS I-V characteristic Practice useful method for solving transistor circuits Build.
1 EE40 Summer 2010 Hug EE40 Lecture 17 Josh Hug 8/04/2010.
EE105 Fall 2011Lecture 6, Slide 1Prof. Salahuddin, UC Berkeley Lecture 6 OUTLINE PN Junction Diodes – Reverse Breakdown – Large and Small signal models.
1 ELE1110D Basic Circuit Theory Tutorial 6 Diode Circuits By Xu Ceng SHB 832.
Lecture 241 Circuits with Dependent Sources Strategy: Apply KVL and KCL, treating dependent source(s) as independent sources. Determine the relationship.
Dr. Nasim Zafar Electronics 1 EEE 231 – BS Electrical Engineering Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
Analysis of Circuits Containing Diodes. Definition of Diode Current and Voltage Forward Bias –When I D > 0mA and V D > 0V Reverse Bias –When I D < 0mA.
Ideal Diode Equation. Important Points of This Lecture There are several different techniques that can be used to determine the diode voltage and current.
10/1/2004EE 42 fall 2004 lecture 141 Lecture #14 Example circuits, Zener diodes, dependent sources, basic amplifiers Reading: 4.10, 5.1, 5.8 Next: transistors.
Dr. Nasim Zafar Electronics 1 - EEE 231 Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
9/13/2004EE 42 fall 2004 lecture 6 Lecture #6 methods of solving circuits Nodal analysis Graphical analysis In the next lecture we will look at circuits.
Circuit Analysis of Circuits Containing Diodes. Definition of Diode Current and Voltage Forward Bias ▫When I D > 0mA and V D > 0V Reverse Bias ▫When I.
09/16/2010© 2010 NTUST Today Course overview and information.
Diodes 1. Basic diode concept. 2. Load-line analysis of diode circuit.
9/27/2004EE 42 fall 2004 lecture 121 Lecture #12 Circuit models for Diodes, Power supplies Reading: Malvino chapter 3, Next: 4.10, 5.1, 5.8 Then.
C H A P T E R 4 Diodes (non-linear devices)
COMSATS Institute of Information Technology Virtual campus Islamabad
ELECTRICA L ENGINEERING Principles and Applications SECOND EDITION ALLAN R. HAMBLEY ©2002 Prentice-Hall, Inc. Chapter 10 Diodes Chapter 10 Diodes 1. Understand.
ELECTRICAL ENGINEERING: PRINCIPLES AND APPLICATIONS, Fourth Edition, by Allan R. Hambley, ©2008 Pearson Education, Inc. Lecture 24 Basic Diode Concepts.
ECE 342 – Jose Schutt-Aine 1 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois 1 ECE 342 Solid-State.
EE 334 Midterm Review. Diode: Why we need to understand diode? The base emitter junction of the BJT behaves as a forward bias diode in amplifying applications.
Recall-Lecture 4 Current generated due to two main factors
ELECTRICAL ENGINEERING: PRINCIPLES AND APPLICATIONS, Third Edition, by Allan R. Hambley, ©2005 Pearson Education, Inc. Chapter 10 Diodes.
MALVINO Electronic PRINCIPLES SIXTH EDITION.
Linear Systems of Equations Section 3.1. What is a “system” of equations?
1 DC Imperfections: Input bias current: Input offset current:
Chapter 10 Diodes. 1. Understand diode operation and select diodes for various applications. 2. Analyze nonlinear circuits using the graphical load-line.
Voltage Regulator Circuits
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. MALVINO & BATES SEVENTH EDITION Electronic PRINCIPLES.
Solving Systems of Equations
Section 4.2 Solving Systems of Equations by Substitution.
Diode Circuit Analysis Techniques Section 4.3. In this Lecture, we will:  Examine dc analysis techniques for diode circuits using various models to describe.
2. Diodes – Basic Diode Concepts 2.1 Basic Diode Concepts Intrinsic Semiconductors * Energy Diagrams – Insulator, Semiconductor, and Conductor the.
EXAMPLE 1 Solve a system graphically Graph the linear system and estimate the solution. Then check the solution algebraically. 4x + y = 8 2x – 3y = 18.
Response of First Order RL and RC
Instantaneous Power (Anlık Güç) Instantaneous power for a 2-terminal element: Instantaneous power for an (n+1)-terminal or n-port element: Total instantaneous.
A Requirement for Superposition. Objective of Lecture Introduce the property of linearity Chapter 4.2.
Diode Circuit Analysis
Example Consider a silicon diode with n =1.5. Find the change in voltage if the current changes from 0.1mA to 10mA.
CSE251 Lecture3 Semiconductor Diodes.
Chapter 3 – Diode Circuits – Part 2
Diode Theory Chapter 3. Copyright © The McGraw-Hill Companies, Inc., Permission required for reproduction or display Topics Covered in Chapter 3 Schematic.
Lecture 16 Today we will Learn how to solve diode circuits
Lecture #14 OUTLINE Midterm #1 stats The pn Junction Diode
Solving Nonlinear Systems
Diode Equation and Models
Transistor Circuit Design Diode Approximations Heathkit EB-6002.
Solve a system of linear equation in two variables
Systems of Linear and Quadratic Equations
Electronic PRINCIPLES
Solving Systems of Linear and Quadratic Equations
Systems of Equations Solve by Graphing.
Linear and Nonlinear Systems of Equations
Linear and Nonlinear Systems of Equations
The Ideal Diode Diodes: The most fundamental non-linear circuit element. The most simple non-linear circuit element. A) The (Ideal) Diode Symbol Notes:
Simple circuit consisting of a source, a resistor, and a diode.
Use Graphs of Functions
Chapter 3 Solid-State Diodes and Diode Circuits
Presentation transcript:

S. RossEECS 40 Spring 2003 Lecture 14 Last time… I V +_+_ Reverse breakdown Reverse bias Forward bias I V ZK VFVF V Focus we introduced the diode and its (complicated) I-V relationship. Today we will… focus on the relevant area of the diode I-V graph develop simpler models for the diode I-V relationship learn how to solve circuits with nonlinear elements

S. RossEECS 40 Spring 2003 Lecture 14 DIFFERENT MODELS, DIFFERENT USES We will consider 4 different diode I-V models with varying degrees of detail. Use most realistic model only for very precise calculations Use simpler models to find basic operation, gain intuition Sometimes one model may lead to an “impossible” situation: use a different (more realistic) model in this case

S. RossEECS 40 Spring 2003 Lecture 14 REALISTIC DIODE MODEL I V I V +_+_ Here, V T is “thermal voltage”: V T = (kT)/q ≈ o K (q is electron charge in C, k is Boltzmann’s constant, and T is the operating temperature in o K) Equation is valid for all modes of operation considered You might need a computer to solve the nonlinear equation this model can create

S. RossEECS 40 Spring 2003 Lecture 14 IDEAL DIODE MODEL I V +_+_ V I Reverse bias Forward bias I V +_+_ Diode either has negative voltage and zero current, or zero voltage and positive current Diode behaves like a switch: open in reverse bias mode, closed (short circuit) in forward bias mode Guess which situation diode is in, see if answer makes sense

S. RossEECS 40 Spring 2003 Lecture 14 LARGE-SIGNAL DIODE MODEL I V +_+_ V I Reverse bias Forward bias I V Diode either has voltage less than V F and zero current, or voltage equal to V F and positive current Diode behaves like a voltage source and switch: open in reverse bias mode, closed in forward bias mode Guess which situation diode is in, see if answer makes sense VFVF VFVF

S. RossEECS 40 Spring 2003 Lecture 14 SMALL-SIGNAL DIODE MODEL I V +_+_ V I Reverse bias Forward bias I V Diode either has voltage less than V F and zero current, or voltage greater than V F and positive current depending on V Diode behaves like a voltage source, resistor and switch: open in reverse bias mode, closed in forward bias mode Guess which situation diode is in, see if answer makes sense VFVF VFVF RDRD slope = 1/R D

S. RossEECS 40 Spring 2003 Lecture 14 SOLVING CIRCUITS WITH NONLINEAR ELEMENTS Look at circuits with a nonlinear element like this: Linear circuit ILIL +VL-+VL- Nonlinear element I NL + V NL - A nonlinear element with its own I-V relationship, attached to a linear circuit with its own I-V relationship. Equations we get: 1.I L = f L (V L )(linear circuit I-V relationship) 2.I NL = f NL (V NL ) (nonlinear element I-V relationship) 3.I NL = -I L 4.V NL = V L

S. RossEECS 40 Spring 2003 Lecture 14 SOLVING CIRCUITS WITH NONLINEAR ELEMENTS Our 4 equations 1.I L = f(V L )(linear circuit I-V relationship) 2.I NL = g(V NL ) (nonlinear element I-V relationship) 3.I NL = -I L 4.V NL = V L can easily become just 2 equations in I NL and V NL 1.I NL = -f L (V NL ) 2.I NL = f NL (V NL ) which we can equate and solve for V NL, or… graph the two equations and solve for the intersection.

S. RossEECS 40 Spring 2003 Lecture 14 LOAD LINE ANALYSIS To find the solution graphically, V NL I NL graph the nonlinear I-V relationship, graph the linear I-V relationship in terms of I NL and V NL (reflect over y-axis), f NL (V NL ) -f L (V NL ) and find the intersection: the voltage across and current through the nonlinear element. x

S. RossEECS 40 Spring 2003 Lecture 14 EXAMPLE +-+- I NL V NL +_+_ 2 V 1 k  VLVL +_+_ ILIL Find V NL. Assume realistic diode model with I 0 = A. 1.I L = (V L - 2) / I NL = -I L 4.V NL = V L Either substitute into 3. and solve or determine graphically that V NL = V

S. RossEECS 40 Spring 2003 Lecture 14

S. RossEECS 40 Spring 2003 Lecture 14 EXAMPLE REVISITED +-+- I NL V NL +_+_ 2 V 1 k  VLVL +_+_ ILIL Find V NL. Assume small-signal diode model with V F = 0.7 V and R D = 20 . 1.I L = (V L - 2) / I NL = (V NL – 0.7) / 20 or I NL = 0 3.I NL = -I L 4.V NL = V L Either substitute into 3. and solve (V NL – 0.7) / 20 = -(V NL - 2) / 1000 or determine graphically that V NL = V

S. RossEECS 40 Spring 2003 Lecture 14

S. RossEECS 40 Spring 2003 Lecture 14 ONE MORE TIME +-+- I NL V NL +_+_ -2 V 1 k  VLVL +_+_ ILIL Find V NL. Assume small-signal diode model with V F = 0.7 V and R D = 20 . 1.I L = (V L - - 2) / I NL = (V NL – 0.7) / 20 or I NL = 0 3.I NL = -I L 4.V NL = V L Either substitute into 3. and solve 0 = -(V NL - - 2) / 1000 or determine graphically that V NL = -2 V

S. RossEECS 40 Spring 2003 Lecture 14