Circuit Analysis with Dependent Sources A)Node Equations B)Equivalent Sources C)Amplifier Parameters: Gain, R IN, R OUT D)Non-Ideal Op-Amp Model

Size: px
Start display at page:

Download "Circuit Analysis with Dependent Sources A)Node Equations B)Equivalent Sources C)Amplifier Parameters: Gain, R IN, R OUT D)Non-Ideal Op-Amp Model"

Transcription

1 Lecture 13: October 15, 2001 Lecture 14: 10/15/01 A.. Neureuther Circuit Analysis with Dependent Sources A)Node Equations B)Equialent Sources C)Amplifier Parameters: Gain,, OUT D)NonIdeal OpAmp Model The following slides were deried from those prepared by Professor Oldham For EE 40 in Fall 01 eading: Schwarz and Oldham Copyright 2001, egents of Uniersity of California

2 Lecture 14: 10/15/01 A.. Neureuther The 4 Basic Linear Dependent Sources Constant of proportionality Parameter being sensed Output Voltagecontrolled oltage source V = A V cd Currentcontrolled oltage source V = m I c Currentcontrolled current source I = A i I c Voltagecontrolled current source I = G m V cd A V cd m I c A i I c G m V cd Copyright 2001, egents of Uniersity of California

3 Lecture 14: 10/15/01 A.. Neureuther EXAMPLE OF NODAL ANALYSIS WITH DEPENDENT SOUCES 1 V a 3 V b I I m I 2 I Standard technique, except an additional equation is needed if the dependent ariable is an unknown current as here. Note Vb is redundant. I = V a / 2 (V a m I 2 )/ 3 and I 2 = V a / 2 Soling: I = V a (1/ 2 1/ 3 m / 2 3 ) So V a = I 2 3 /( 2 3 m ) Copyright 2001, egents of Uniersity of California

4 Lecture 14: 10/15/01 A.. Neureuther THEVEN EQUIVALENT WITH DEPENDENT SOUCES Method 1: Use V oc and I sc as usual to find V T and T (and I N as well) Method 2: To find T by the ohmmeter method turn off only the independent sources; let the dependent sources just do their thing. See examples in text (such as Example 4.3). This method also works when computing incremental signals such as a change in the source V S (gien by V S or S ) produces a change in V or V OUT, (gien by V or V OUT also written and OUT ), and their ratio called the smallsignal gain ( V OUT / V S ) or ( OUT / S ) Copyright 2001, egents of Uniersity of California

5 Lecture 14: 10/15/01 A.. Neureuther EXAMPLE CICUIT WITH MULTIPLE SOUCES Original circuit s a V b L V DD Vs G m V b V V DD V OUT O Circuit with independent sources turned to zero s G m s b a OUT O L Note L has been rotated down. Copyright 2001, egents of Uniersity of California

6 Lecture 14: 10/15/01 A.. Neureuther EXAMPLE CICUIT: GA = ( V OUT / V S )=( OUT/ S ) s G m s b a O L OUT OUT a b = = s a b S = G m O O L L = G m S O O L L S Input oltage diider and output current diider reduce the gain Copyright 2001, egents of Uniersity of California

7 Lecture 14: 10/15/01 A.. Neureuther EXAMPLE CICUIT: PUT/OUTPUT ESISTANCE s G m s b a O L OUT = a a OUT = O b b Deice Output does not feed back to input Assume S = 0 => = 0 => no current in dependent source OUT Can circuit design improe and OUT or do we need better deices? Copyright 2001, egents of Uniersity of California

8 Lecture 14: 10/15/01 A.. Neureuther EXAMPLE CICUIT: CEASED PUT ESISTANCE i TEST Add resistor E TEST E G m O The output has been assumed to be shorted OUT = 0 E Analysis: apply i TEST and ealuate TEST KCL = E E Check for special case for 0 infinite i TEST = i TEST E itest GmiTEST 0 i TEST TEST = ( 1 G TEST Copyright 2001, egents of Uniersity of California m = 0 ) E E Finish this in the homework Intuitie Explanation: E puts on a node whose oltage increases in response to current in.

9 Lecture 14: 10/15/01 A.. Neureuther EXAMPLE CICUIT: CEASED OUTPUT ESISTANCE i TEST Add resistor E G m = 0 The input has been assumed to be shorted E E O TEST Try a bag. It is een easier Analysis: apply i TEST and ealuate TEST Unknowns: i TEST, TEST,, E Need 3 equations to find the ratio of i TEST / TEST Intuitie Explanation: GmV burps current which has to also go through 0. This raises TEST and the output impedance TEST /i TEST = E and is not zero! KCL at E KVL at OUT Finish this in the homework Copyright 2001, egents of Uniersity of California

10 NONIDEAL OPAMPS Lecture 14: 10/15/01 A.. Neureuther JUST ANOTHE CASE OF ANALYSIS WITH DEPENDENT SOUCES Example: Circuit (assume ) 1 2 1K V 9K V 0 1 1K V ( ) () 2 9K V 0 A (V V ) Analysis: Outline your circuit analysis strategy here. Hint: 1) Find V in terms of V 0, 2) plug into expression for V 0 and then 3) sole for V 0 which appears on both sides of the equation. Answer: V 0 = V A( 1 (A 1) 1 2 ) 2 V if A = 10V Copyright 2001, egents of Uniersity of California

EECS 42 Spring 2001 Lecture 14. W. G. Oldham MORE NODAL ANALYSIS. Today: Dependent Sources Examples

EECS 42 Spring 2001 Lecture 14. W. G. Oldham MORE NODAL ANALYSIS. Today: Dependent Sources Examples MOE NODAL ANALYSIS Today: Dependent Sources Examples 1 Dependent oltage and Current Sources A linear dependent source is a voltage or current source that depends linearly on some other circuit current

More information

Lecture 8: 09/18/03 A.R. Neureuther Version Date 09/14/03 EECS 42 Introduction Digital Electronics Andrew R. Neureuther

Lecture 8: 09/18/03 A.R. Neureuther Version Date 09/14/03 EECS 42 Introduction Digital Electronics Andrew R. Neureuther EECS ntroduction Digital Electronics ndrew. Neureuther Lecture #8 Node Equations Systematic Node Equations Example: oltage and Current Dividers Example 5 Element Circuit Schwarz and Oldham 5-58,.5, &.6

More information

EE40. Lec 3. Basic Circuit Analysis. Prof. Nathan Cheung. Reading: Hambley Chapter 2

EE40. Lec 3. Basic Circuit Analysis. Prof. Nathan Cheung. Reading: Hambley Chapter 2 EE40 Lec 3 Basic Circuit Analysis Prof. Nathan Cheung 09/03/009 eading: Hambley Chapter Slide Outline Chapter esistors in Series oltage Divider Conductances in Parallel Current Divider Node-oltage Analysis

More information

Lecture 7: September 19th, The following slides were derived from those prepared by Professor Oldham for EE40 in Fall 01. Version Date 9/19/01

Lecture 7: September 19th, The following slides were derived from those prepared by Professor Oldham for EE40 in Fall 01. Version Date 9/19/01 EES Intro. electronics for S Fall Lecture 7: September 9th, Lecture 7: 9/9/ A.. Neureuther Version Date 9/9/ harging and Discharging of ircuits (Transients) A) Mathematical Method B) EE Easy Method ) Logic

More information

Chapter 5 Solution P5.2-2, 3, 6 P5.3-3, 5, 8, 15 P5.4-3, 6, 8, 16 P5.5-2, 4, 6, 11 P5.6-2, 4, 9

Chapter 5 Solution P5.2-2, 3, 6 P5.3-3, 5, 8, 15 P5.4-3, 6, 8, 16 P5.5-2, 4, 6, 11 P5.6-2, 4, 9 Chapter 5 Solution P5.2-2, 3, 6 P5.3-3, 5, 8, 15 P5.4-3, 6, 8, 16 P5.5-2, 4, 6, 11 P5.6-2, 4, 9 P 5.2-2 Consider the circuit of Figure P 5.2-2. Find i a by simplifying the circuit (using source transformations)

More information

1 S = G R R = G. Enzo Paterno

1 S = G R R = G. Enzo Paterno ECET esistie Circuits esistie Circuits: - Ohm s Law - Kirchhoff s Laws - Single-Loop Circuits - Single-Node Pair Circuits - Series Circuits - Parallel Circuits - Series-Parallel Circuits Enzo Paterno ECET

More information

Lecture 10: 09//25/03 A.R. Neureuther Version Date 09/14/03 EECS 42 Introduction to Digital Electronics Andrew R. Neureuther

Lecture 10: 09//25/03 A.R. Neureuther Version Date 09/14/03 EECS 42 Introduction to Digital Electronics Andrew R. Neureuther EECS 42 Intro. Digital Electronics Fall 23 Lecture : 9//25/3.R. Neureuther Version Date 9/4/3 EECS 42 Introduction to Digital Electronics ndrew R. Neureuther Lecture # Prof. King: asic Digital locks 2

More information

Chapter 10 AC Analysis Using Phasors

Chapter 10 AC Analysis Using Phasors Chapter 10 AC Analysis Using Phasors 10.1 Introduction We would like to use our linear circuit theorems (Nodal analysis, Mesh analysis, Thevenin and Norton equivalent circuits, Superposition, etc.) to

More information

ELECTRONIC DEVICES. Assist. prof. Laura-Nicoleta IVANCIU, Ph.D. C1 Introduction. Fundamentals.

ELECTRONIC DEVICES. Assist. prof. Laura-Nicoleta IVANCIU, Ph.D. C1 Introduction. Fundamentals. ELETRONI DEVIES Assist. prof. Laura-Nicoleta IVANIU, Ph.D. Introduction.. Introduction.. ontents ourse presentation Desired outcome. Ealuation. Laura-Nicoleta IVANIU, Electronic deices 2 Introduction..

More information

In this lecture, we will consider how to analyse an electrical circuit by applying KVL and KCL. As a result, we can predict the voltages and currents

In this lecture, we will consider how to analyse an electrical circuit by applying KVL and KCL. As a result, we can predict the voltages and currents In this lecture, we will consider how to analyse an electrical circuit by applying KVL and KCL. As a result, we can predict the voltages and currents around an electrical circuit. This is a short lecture,

More information

EE 247B/ME 218: Introduction to MEMS Design Lecture 26m1: Noise & MDS CTN 4/25/17. Copyright 2017 Regents of the University of California

EE 247B/ME 218: Introduction to MEMS Design Lecture 26m1: Noise & MDS CTN 4/25/17. Copyright 2017 Regents of the University of California EE 47B/ME 18: Introduction to MEMS Design Lecture 6m1: & MDS CTN 4/5/17 Thermal Sources Thermal in Electronics: (Johnson noise, Nyquist noise) Produced as a result of the thermally excited random motion

More information

LECTURE 2: CROSS PRODUCTS, MULTILINEARITY, AND AREAS OF PARALLELOGRAMS

LECTURE 2: CROSS PRODUCTS, MULTILINEARITY, AND AREAS OF PARALLELOGRAMS LECTURE : CROSS PRODUCTS, MULTILINEARITY, AND AREAS OF PARALLELOGRAMS MA1111: LINEAR ALGEBRA I, MICHAELMAS 016 1. Finishing up dot products Last time we stated the following theorem, for which I owe you

More information

Chapter 2 Resistive Circuits

Chapter 2 Resistive Circuits 1. Sole circuits (i.e., find currents and oltages of interest) by combining resistances in series and parallel. 2. Apply the oltage-diision and current-diision principles. 3. Sole circuits by the node-oltage

More information

Midterm Exam (closed book/notes) Tuesday, February 23, 2010

Midterm Exam (closed book/notes) Tuesday, February 23, 2010 University of California, Berkeley Spring 2010 EE 42/100 Prof. A. Niknejad Midterm Exam (closed book/notes) Tuesday, February 23, 2010 Guidelines: Closed book. You may use a calculator. Do not unstaple

More information

Chapter 4: Techniques of Circuit Analysis

Chapter 4: Techniques of Circuit Analysis Chapter 4: Techniques of Circuit Analysis This chapter gies us many useful tools for soling and simplifying circuits. We saw a few simple tools in the last chapter (reduction of circuits ia series and

More information

Chapter 3 Methods of Analysis: 1) Nodal Analysis

Chapter 3 Methods of Analysis: 1) Nodal Analysis Chapter 3 Methods of Analysis: 1) Nodal Analysis Dr. Waleed Al-Hanafy waleed alhanafy@yahoo.com Faculty of Electronic Engineering, Menoufia Univ., Egypt MSA Summer Course: Electric Circuit Analysis I (ESE

More information

09-Circuit Theorems Text: , 4.8. ECEGR 210 Electric Circuits I

09-Circuit Theorems Text: , 4.8. ECEGR 210 Electric Circuits I 09Circuit Theorems Text: 4.1 4.3, 4.8 ECEGR 210 Electric Circuits I Overview Introduction Linearity Superposition Maximum Power Transfer Dr. Louie 2 Introduction Nodal and mesh analysis can be tedious

More information

Electric Circuits I. Nodal Analysis. Dr. Firas Obeidat

Electric Circuits I. Nodal Analysis. Dr. Firas Obeidat Electric Circuits I Nodal Analysis Dr. Firas Obeidat 1 Nodal Analysis Without Voltage Source Nodal analysis, which is based on a systematic application of Kirchhoff s current law (KCL). A node is defined

More information

Chapter 2 Resistive Circuits

Chapter 2 Resistive Circuits Chapter esistie Circuits Goal. Sole circuits by combining resistances in Series and Parallel.. Apply the Voltage-Diision and Current-Diision Principles.. Sole circuits by the Node-Voltage Technique.. Sole

More information

D is the voltage difference = (V + - V - ).

D is the voltage difference = (V + - V - ). 1 Operational amplifier is one of the most common electronic building blocks used by engineers. It has two input terminals: V + and V -, and one output terminal Y. It provides a gain A, which is usually

More information

Chapter 10 Sinusoidal Steady State Analysis Chapter Objectives:

Chapter 10 Sinusoidal Steady State Analysis Chapter Objectives: Chapter 10 Sinusoidal Steady State Analysis Chapter Objectives: Apply previously learn circuit techniques to sinusoidal steady-state analysis. Learn how to apply nodal and mesh analysis in the frequency

More information

Chapter 10: Sinusoidal Steady-State Analysis

Chapter 10: Sinusoidal Steady-State Analysis Chapter 10: Sinusoidal Steady-State Analysis 10.1 10.2 10.3 10.4 10.5 10.6 10.9 Basic Approach Nodal Analysis Mesh Analysis Superposition Theorem Source Transformation Thevenin & Norton Equivalent Circuits

More information

EE292: Fundamentals of ECE

EE292: Fundamentals of ECE EE292: Fundamentals of ECE Fall 2012 TTh 10:00-11:15 SEB 1242 Lecture 4 120906 http://www.ee.unlv.edu/~b1morris/ee292/ 2 Outline Review Voltage Divider Current Divider Node-Voltage Analysis 3 Network Analysis

More information

Lecture #3. Review: Power

Lecture #3. Review: Power Lecture #3 OUTLINE Power calculations Circuit elements Voltage and current sources Electrical resistance (Ohm s law) Kirchhoff s laws Reading Chapter 2 Lecture 3, Slide 1 Review: Power If an element is

More information

A tricky node-voltage situation

A tricky node-voltage situation A tricky node-voltage situation The node-method will always work you can always generate enough equations to determine all of the node voltages. The method we have outlined well in almost all cases, but

More information

Electronics II. Final Examination

Electronics II. Final Examination The University of Toledo f17fs_elct27.fm 1 Electronics II Final Examination Problems Points 1. 11 2. 14 3. 15 Total 40 Was the exam fair? yes no The University of Toledo f17fs_elct27.fm 2 Problem 1 11

More information

ECE 1311: Electric Circuits. Chapter 2: Basic laws

ECE 1311: Electric Circuits. Chapter 2: Basic laws ECE 1311: Electric Circuits Chapter 2: Basic laws Basic Law Overview Ideal sources series and parallel Ohm s law Definitions open circuits, short circuits, conductance, nodes, branches, loops Kirchhoff's

More information

Solution: Based on the slope of q(t): 20 A for 0 t 1 s dt = 0 for 3 t 4 s. 20 A for 4 t 5 s 0 for t 5 s 20 C. t (s) 20 C. i (A) Fig. P1.

Solution: Based on the slope of q(t): 20 A for 0 t 1 s dt = 0 for 3 t 4 s. 20 A for 4 t 5 s 0 for t 5 s 20 C. t (s) 20 C. i (A) Fig. P1. Problem 1.24 The plot in Fig. P1.24 displays the cumulative charge q(t) that has entered a certain device up to time t. Sketch a plot of the corresponding current i(t). q 20 C 0 1 2 3 4 5 t (s) 20 C Figure

More information

EE243 Advanced Electromagnetic Theory Lec # 15 Plasmons. Reading: These PPT notes and Harrington on corrugated surface 4.8.

EE243 Advanced Electromagnetic Theory Lec # 15 Plasmons. Reading: These PPT notes and Harrington on corrugated surface 4.8. EE Applied EM Fall 6, Neureuther Lecture #5 Ver //6 EE43 Adanced Electromagnetic Theory Lec # 5 Plasmons Fixed Slides 6, (Group and Phase Velocity for Guided Waes) (Sign Reersals for Propagation Direction

More information

Sinusoidal Steady State Analysis (AC Analysis) Part I

Sinusoidal Steady State Analysis (AC Analysis) Part I Sinusoidal Steady State Analysis (AC Analysis) Part I Amin Electronics and Electrical Communications Engineering Department (EECE) Cairo University elc.n102.eng@gmail.com http://scholar.cu.edu.eg/refky/

More information

EXPERIMENT THREE DC CIRCUITS

EXPERIMENT THREE DC CIRCUITS EXEMET THEE DC CCUT EQUMET EEDED: ) DC ower upply ) DMM 3) esistors 4) EL THEOY Kirchhoff's Laws: Kirchhoff's oltage Law: The algebraic sum of the voltages around any closed path is zero. v i i 0 3. Kirchhoff's

More information

dv dv 2 2 dt dt dv dt

dv dv 2 2 dt dt dv dt 1/3/14 hapter 8 Second order circuits A circuit with two energy storage elements: One inductor, one capacitor Two capacitors, or Two inductors i Such a circuit will be described with second order differential

More information

Physics 1402: Lecture 10 Today s Agenda

Physics 1402: Lecture 10 Today s Agenda Physics 1402: Lecture 10 Today s Agenda Announcements: Lectures posted on: www.phys.uconn.edu/~rcote/ HW assignments, solutions etc. Homework #3: On Masterphysics : due Friday at 8:00 AM Go to masteringphysics.com

More information

Chapter 5. Department of Mechanical Engineering

Chapter 5. Department of Mechanical Engineering Source Transformation By KVL: V s =ir s + v By KCL: i s =i + v/r p is=v s /R s R s =R p V s /R s =i + v/r s i s =i + v/r p Two circuits have the same terminal voltage and current Source Transformation

More information

Sinusoidal Steady State Analysis (AC Analysis) Part II

Sinusoidal Steady State Analysis (AC Analysis) Part II Sinusoidal Steady State Analysis (AC Analysis) Part II Amin Electronics and Electrical Communications Engineering Department (EECE) Cairo University elc.n102.eng@gmail.com http://scholar.cu.edu.eg/refky/

More information

E2.2 Analogue Electronics

E2.2 Analogue Electronics E2.2 Analogue Electronics Instructor : Christos Papavassiliou Office, email : EE 915, c.papavas@imperial.ac.uk Lectures : Monday 2pm, room 408 (weeks 2-11) Thursday 3pm, room 509 (weeks 4-11) Problem,

More information

Electrical Technology (EE-101-F)

Electrical Technology (EE-101-F) Electrical Technology (EE-101-F) Contents Series & Parallel Combinations KVL & KCL Introduction to Loop & Mesh Analysis Frequently Asked Questions NPTEL Link Series-Parallel esistances 1 V 3 2 There are

More information

Homework 3 Solution. Due Friday (5pm), Feb. 14, 2013

Homework 3 Solution. Due Friday (5pm), Feb. 14, 2013 University of California, Berkeley Spring 2013 EE 42/100 Prof. K. Pister Homework 3 Solution Due Friday (5pm), Feb. 14, 2013 Please turn the homework in to the drop box located next to 125 Cory Hall (labeled

More information

Circuit Theorems Overview Linearity Superposition Source Transformation Thévenin and Norton Equivalents Maximum Power Transfer

Circuit Theorems Overview Linearity Superposition Source Transformation Thévenin and Norton Equivalents Maximum Power Transfer Circuit Theorems Overview Linearity Superposition Source Transformation Thévenin and Norton Equivalents Maximum Power Transfer J. McNames Portland State University ECE 221 Circuit Theorems Ver. 1.36 1

More information

E E 2320 Circuit Analysis. Calculating Resistance

E E 2320 Circuit Analysis. Calculating Resistance E E 30 Circuit Analysis Lecture 03 Simple esistive Circuits it and Applications Calculating esistance l A 6 1.67 10 cm cu 6 al.7010 Area, A When conductor has uniform crosssection cm l 1 Temperature Coefficient

More information

Active Circuits: Life gets interesting

Active Circuits: Life gets interesting Actie Circuits: Life gets interesting Actie cct elements operational amplifiers (OP AMPS) and transistors Deices which can inject power into the cct External power supply normally comes from connection

More information

Delhi Noida Bhopal Hyderabad Jaipur Lucknow Indore Pune Bhubaneswar Kolkata Patna Web: Ph:

Delhi Noida Bhopal Hyderabad Jaipur Lucknow Indore Pune Bhubaneswar Kolkata Patna Web:     Ph: Serial : CH_EE_B_Network Theory_098 Delhi Noida Bhopal Hyderabad Jaipur Lucknow ndore Pune Bhubaneswar Kolkata Patna Web: E-mail: info@madeeasy.in Ph: 0-56 CLASS TEST 08-9 ELECTCAL ENGNEENG Subject : Network

More information

Problem Set 4 Solutions

Problem Set 4 Solutions University of California, Berkeley Spring 212 EE 42/1 Prof. A. Niknejad Problem Set 4 Solutions Please note that these are merely suggested solutions. Many of these problems can be approached in different

More information

Thevenin Norton Equivalencies - GATE Study Material in PDF

Thevenin Norton Equivalencies - GATE Study Material in PDF Thevenin Norton Equivalencies - GATE Study Material in PDF In these GATE 2018 Notes, we explain the Thevenin Norton Equivalencies. Thevenin s and Norton s Theorems are two equally valid methods of reducing

More information

1. Review of Circuit Theory Concepts

1. Review of Circuit Theory Concepts 1. Review of Circuit Theory Concepts Lecture notes: Section 1 ECE 65, Winter 2013, F. Najmabadi Circuit Theory is an pproximation to Maxwell s Electromagnetic Equations circuit is made of a bunch of elements

More information

NODAL ANALYSIS CONTINUED

NODAL ANALYSIS CONTINUED EES 4 Spring 00 Lecture 0 opyright egents of University of alifornia W. G. Oldham NODAL ANALY ONTNUED Lecture 9 review: Formal nodal analysis oltage divider example Today: Nodal analysis with floating

More information

Chapter 2. Engr228 Circuit Analysis. Dr Curtis Nelson

Chapter 2. Engr228 Circuit Analysis. Dr Curtis Nelson Chapter 2 Engr228 Circuit Analysis Dr Curtis Nelson Chapter 2 Objectives Understand symbols and behavior of the following circuit elements: Independent voltage and current sources; Dependent voltage and

More information

Active Circuits: Life gets interesting

Active Circuits: Life gets interesting Actie Circuits: Life gets interesting Actie cct elements operational amplifiers (OP AMPS) and transistors Deices which can inject power into the cct External power supply normally comes from connection

More information

4/27 Friday. I have all the old homework if you need to collect them.

4/27 Friday. I have all the old homework if you need to collect them. 4/27 Friday Last HW: do not need to turn it. Solution will be posted on the web. I have all the old homework if you need to collect them. Final exam: 7-9pm, Monday, 4/30 at Lambert Fieldhouse F101 Calculator

More information

Series & Parallel Resistors 3/17/2015 1

Series & Parallel Resistors 3/17/2015 1 Series & Parallel Resistors 3/17/2015 1 Series Resistors & Voltage Division Consider the single-loop circuit as shown in figure. The two resistors are in series, since the same current i flows in both

More information

Lecture 6: Impedance (frequency dependent. resistance in the s- world), Admittance (frequency. dependent conductance in the s- world), and

Lecture 6: Impedance (frequency dependent. resistance in the s- world), Admittance (frequency. dependent conductance in the s- world), and Lecture 6: Impedance (frequency dependent resistance in the s- world), Admittance (frequency dependent conductance in the s- world), and Consequences Thereof. Professor Ray, what s an impedance? Answers:

More information

ECE 212H1F Circuit Analysis October 20, :15-19: Reza Iravani 02 Reza Iravani 03 Ali Nabavi-Niaki. (Non-programmable Calculators Allowed)

ECE 212H1F Circuit Analysis October 20, :15-19: Reza Iravani 02 Reza Iravani 03 Ali Nabavi-Niaki. (Non-programmable Calculators Allowed) Please Print Clearly Last Name: First Name: Student Number: Your Tutorial Section (CIRCLE ONE): 01 Thu 10:00 12:00 HA403 02 Thu 10:00 12:00 GB412 03 Thu 15:00 17:00 GB412 04 Thu 15:00 17:00 SF2202 05 Fri

More information

DC STEADY STATE CIRCUIT ANALYSIS

DC STEADY STATE CIRCUIT ANALYSIS DC STEADY STATE CIRCUIT ANALYSIS 1. Introduction The basic quantities in electric circuits are current, voltage and resistance. They are related with Ohm s law. For a passive branch the current is: I=

More information

Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science : Circuits & Electronics Problem Set #1 Solution

Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science : Circuits & Electronics Problem Set #1 Solution Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science 6.2: Circuits & Electronics Problem Set # Solution Exercise. The three resistors form a series connection.

More information

Lecture 3 BRANCHES AND NODES

Lecture 3 BRANCHES AND NODES Lecture 3 Definitions: Circuits, Nodes, Branches Kirchoff s Voltage Law (KVL) Kirchoff s Current Law (KCL) Examples and generalizations RC Circuit Solution 1 Branch: BRANCHES AND NODES elements connected

More information

Problem Set 5 Solutions

Problem Set 5 Solutions University of California, Berkeley Spring 01 EE /0 Prof. A. Niknejad Problem Set 5 Solutions Please note that these are merely suggested solutions. Many of these problems can be approached in different

More information

MAE140 - Linear Circuits - Winter 09 Midterm, February 5

MAE140 - Linear Circuits - Winter 09 Midterm, February 5 Instructions MAE40 - Linear ircuits - Winter 09 Midterm, February 5 (i) This exam is open book. You may use whatever written materials you choose, including your class notes and textbook. You may use a

More information

MAE140 - Linear Circuits - Fall 14 Midterm, November 6

MAE140 - Linear Circuits - Fall 14 Midterm, November 6 MAE140 - Linear Circuits - Fall 14 Midterm, November 6 Instructions (i) This exam is open book. You may use whatever written materials you choose, including your class notes and textbook. You may use a

More information

Textbook title: Circuits, Devices, Networks and Microelectronics

Textbook title: Circuits, Devices, Networks and Microelectronics Circuits, Deices, Networks and Microelectronics Textbook title: Circuits, Deices, Networks and Microelectronics CHAPTE 5. THE IDEAL OPAMP 5. THE OPEATIONAL AMPLIFIE, CONTEXT and QUALIFICATION The operational

More information

Chapter 2 Circuit Elements

Chapter 2 Circuit Elements Chapter 2 Circuit Elements 2.1 Voltage and Current Sources 2.2 Electrical Resistance (Ohm s Law) 2.3 Construction of a Circuit Model 2.4 Kirchhoff s Laws 2.5 Analysis of a Circuit Containing Dependent

More information

Designing Information Devices and Systems II Fall 2016 Murat Arcak and Michel Maharbiz Homework 0. This homework is due August 29th, 2016, at Noon.

Designing Information Devices and Systems II Fall 2016 Murat Arcak and Michel Maharbiz Homework 0. This homework is due August 29th, 2016, at Noon. EECS 16B Designing Information Devices and Systems II Fall 2016 Murat Arcak and Michel Maharbiz Homework 0 This homework is due August 29th, 2016, at Noon. 1. Homework process and study group (a) Who else

More information

Designing Information Devices and Systems I Spring 2018 Lecture Notes Note 20

Designing Information Devices and Systems I Spring 2018 Lecture Notes Note 20 EECS 16A Designing Information Devices and Systems I Spring 2018 Lecture Notes Note 20 Design Example Continued Continuing our analysis for countdown timer circuit. We know for a capacitor C: I = C dv

More information

Lecture 37: Frequency response. Context

Lecture 37: Frequency response. Context EECS 05 Spring 004, Lecture 37 Lecture 37: Frequency response Prof J. S. Smith EECS 05 Spring 004, Lecture 37 Context We will figure out more of the design parameters for the amplifier we looked at in

More information

FE Review 2/2/2011. Electric Charge. Electric Energy ELECTRONICS # 1 FUNDAMENTALS

FE Review 2/2/2011. Electric Charge. Electric Energy ELECTRONICS # 1 FUNDAMENTALS FE eview ELECONICS # FUNDAMENALS Electric Charge 2 In an electric circuit there is a conservation of charge. he net electric charge is constant. here are positive and negative charges. Like charges repel

More information

Review of Circuit Analysis

Review of Circuit Analysis Review of Circuit Analysis Fundamental elements Wire Resistor Voltage Source Current Source Kirchhoff s Voltage and Current Laws Resistors in Series Voltage Division EE 42 Lecture 2 1 Voltage and Current

More information

A tricky node-voltage situation

A tricky node-voltage situation A tricky node-voltage situation The node-method will always work you can always generate enough equations to determine all of the node voltages. The prescribed method quite well, but there is one situation

More information

Chapter 4 Homework solution: P4.2-2, 7 P4.3-2, 3, 6, 9 P4.4-2, 5, 8, 18 P4.5-2, 4, 5 P4.6-2, 4, 8 P4.7-2, 4, 9, 15 P4.8-2

Chapter 4 Homework solution: P4.2-2, 7 P4.3-2, 3, 6, 9 P4.4-2, 5, 8, 18 P4.5-2, 4, 5 P4.6-2, 4, 8 P4.7-2, 4, 9, 15 P4.8-2 Chpter 4 Homework solution: P4.2-2, 7 P4.3-2, 3, 6, 9 P4.4-2, 5, 8, 18 P4.5-2, 4, 5 P4.6-2, 4, 8 P4.7-2, 4, 9, 15 P4.8-2 P 4.2-2 P 4.2-2. Determine the node voltges for the circuit of Figure Answer: v

More information

Module 2. DC Circuit. Version 2 EE IIT, Kharagpur

Module 2. DC Circuit. Version 2 EE IIT, Kharagpur Module 2 DC Circuit Lesson 5 Node-voltage analysis of resistive circuit in the context of dc voltages and currents Objectives To provide a powerful but simple circuit analysis tool based on Kirchhoff s

More information

Notes for course EE1.1 Circuit Analysis TOPIC 10 2-PORT CIRCUITS

Notes for course EE1.1 Circuit Analysis TOPIC 10 2-PORT CIRCUITS Objectives: Introduction Notes for course EE1.1 Circuit Analysis 4-5 Re-examination of 1-port sub-circuits Admittance parameters for -port circuits TOPIC 1 -PORT CIRCUITS Gain and port impedance from -port

More information

EE 40: Introduction to Microelectronic Circuits Spring 2008: Midterm 2

EE 40: Introduction to Microelectronic Circuits Spring 2008: Midterm 2 EE 4: Introduction to Microelectronic Circuits Spring 8: Midterm Venkat Anantharam 3/9/8 Total Time Allotted : min Total Points:. This is a closed book exam. However, you are allowed to bring two pages

More information

Review of Ohm's Law: The potential drop across a resistor is given by Ohm's Law: V= IR where I is the current and R is the resistance.

Review of Ohm's Law: The potential drop across a resistor is given by Ohm's Law: V= IR where I is the current and R is the resistance. DC Circuits Objectives The objectives of this lab are: 1) to construct an Ohmmeter (a device that measures resistance) using our knowledge of Ohm's Law. 2) to determine an unknown resistance using our

More information

Phasors: Impedance and Circuit Anlysis. Phasors

Phasors: Impedance and Circuit Anlysis. Phasors Phasors: Impedance and Circuit Anlysis Lecture 6, 0/07/05 OUTLINE Phasor ReCap Capacitor/Inductor Example Arithmetic with Complex Numbers Complex Impedance Circuit Analysis with Complex Impedance Phasor

More information

EE 205 Dr. A. Zidouri. Electric Circuits II. Two-Port Circuits Two-Port Parameters. Lecture #42

EE 205 Dr. A. Zidouri. Electric Circuits II. Two-Port Circuits Two-Port Parameters. Lecture #42 EE 05 Dr. A. Zidouri Electric Circuits Two-Port Circuits Two-Port Parameters Lecture #4-1 - EE 05 Dr. A. Zidouri The material to be covered in this lecture is as follows: o ntroduction to two-port circuits

More information

Designing Information Devices and Systems I Fall 2018 Lecture Notes Note Introduction: Op-amps in Negative Feedback

Designing Information Devices and Systems I Fall 2018 Lecture Notes Note Introduction: Op-amps in Negative Feedback EECS 16A Designing Information Devices and Systems I Fall 2018 Lecture Notes Note 18 18.1 Introduction: Op-amps in Negative Feedback In the last note, we saw that can use an op-amp as a comparator. However,

More information

VV = voltage across voltmeter = 9 (Rs + 500) = VsRv Vs. (500) = 9 (Rs + 500) Case ii VV = 13V VS=? RV = 50kΩ / V 20v RV = 1000 kω by (1)

VV = voltage across voltmeter = 9 (Rs + 500) = VsRv Vs. (500) = 9 (Rs + 500) Case ii VV = 13V VS=? RV = 50kΩ / V 20v RV = 1000 kω by (1) 1 1. A resistor has oltage drop of 110.V and current of.a. the uncertainties in the measurement of oltage and current are ± 0.V and ±0.01 respectiely calculate the uncertainty in power calculation. Ans.

More information

Preamble. Circuit Analysis II. Mesh Analysis. When circuits get really complex methods learned so far will still work,

Preamble. Circuit Analysis II. Mesh Analysis. When circuits get really complex methods learned so far will still work, Preamble Circuit Analysis II Physics, 8 th Edition Custom Edition Cutnell & Johnson When circuits get really complex methods learned so far will still work, but they can take a long time to do. A particularly

More information

Homework 1 solutions

Homework 1 solutions Electric Circuits 1 Homework 1 solutions (Due date: 2014/3/3) This assignment covers Ch1 and Ch2 of the textbook. The full credit is 100 points. For each question, detailed derivation processes and accurate

More information

Electric Circuits II Sinusoidal Steady State Analysis. Dr. Firas Obeidat

Electric Circuits II Sinusoidal Steady State Analysis. Dr. Firas Obeidat Electric Circuits II Sinusoidal Steady State Analysis Dr. Firas Obeidat 1 Table of Contents 1 2 3 4 5 Nodal Analysis Mesh Analysis Superposition Theorem Source Transformation Thevenin and Norton Equivalent

More information

L Hopital s Rule. We will use our knowledge of derivatives in order to evaluate limits that produce indeterminate forms.

L Hopital s Rule. We will use our knowledge of derivatives in order to evaluate limits that produce indeterminate forms. L Hopital s Rule We will use our knowledge of derivatives in order to evaluate its that produce indeterminate forms. Main Idea x c f x g x If, when taking the it as x c, you get an INDETERMINATE FORM..

More information

Designing Information Devices and Systems I Spring 2018 Homework 7

Designing Information Devices and Systems I Spring 2018 Homework 7 EECS 6A Designing Information Devices and Systems I Spring 08 Homework 7 This homework is due March, 08, at 3:59. Self-grades are due March 5, 08, at 3:59. Submission Format Your homework submission should

More information

Lecture Stage Frequency Response - I (1/10/02) Page ECE Analog Integrated Circuits and Systems II P.E.

Lecture Stage Frequency Response - I (1/10/02) Page ECE Analog Integrated Circuits and Systems II P.E. Lecture 070 Stage Frequency esponse I (/0/0) Page 070 LECTUE 070 SINGLESTAGE FEQUENCY ESPONSE I (EADING: GHLM 488504) Objective The objective of this presentation is:.) Illustrate the frequency analysis

More information

L Hopital s Rule. We will use our knowledge of derivatives in order to evaluate limits that produce indeterminate forms.

L Hopital s Rule. We will use our knowledge of derivatives in order to evaluate limits that produce indeterminate forms. L Hopital s Rule We will use our knowledge of derivatives in order to evaluate its that produce indeterminate forms. Indeterminate Limits Main Idea x c f x g x If, when taking the it as x c, you get an

More information

INTRODUCTION TO ELECTRONICS

INTRODUCTION TO ELECTRONICS INTRODUCTION TO ELECTRONICS Basic Quantities Voltage (symbol V) is the measure of electrical potential difference. It is measured in units of Volts, abbreviated V. The example below shows several ways

More information

Outline. Week 5: Circuits. Course Notes: 3.5. Goals: Use linear algebra to determine voltage drops and branch currents.

Outline. Week 5: Circuits. Course Notes: 3.5. Goals: Use linear algebra to determine voltage drops and branch currents. Outline Week 5: Circuits Course Notes: 3.5 Goals: Use linear algebra to determine voltage drops and branch currents. Components in Resistor Networks voltage source current source resistor Components in

More information

Fig. 1-1 Current Flow in a Resistive load

Fig. 1-1 Current Flow in a Resistive load 1 Electric Circuits: Current flow in a resistive load flows either from (-) to () which is labeled below as Electron flow or the Conventional flow from () to (-). We will use conventional flow in this

More information

Consider the following generalized simple circuit

Consider the following generalized simple circuit ntroduction to Circuit Analysis Getting Started We analyze circuits for several reasons Understand how they work Learn how to design from other people s work Debug our own designs Troubleshoot circuit

More information

Chapter 6: Operational Amplifiers

Chapter 6: Operational Amplifiers Chapter 6: Operational Amplifiers Circuit symbol and nomenclature: An op amp is a circuit element that behaes as a VCVS: The controlling oltage is in = and the controlled oltage is such that 5 5 A where

More information

Network Topology-2 & Dual and Duality Choice of independent branch currents and voltages: The solution of a network involves solving of all branch currents and voltages. We know that the branch current

More information

EE292: Fundamentals of ECE

EE292: Fundamentals of ECE EE292: Fundamentals of ECE Fall 2012 TTh 10:00-11:15 SEB 1242 Lecture 14 121011 http://www.ee.unlv.edu/~b1morris/ee292/ 2 Outline Review Steady-State Analysis RC Circuits RL Circuits 3 DC Steady-State

More information

Lecture 18. Common Source Stage

Lecture 18. Common Source Stage ecture 8 OUTINE Basic MOSFET amplifier MOSFET biasing MOSFET current sources Common source amplifier eading: Chap. 7. 7.7. EE05 Spring 008 ecture 8, Slide Prof. Wu, UC Berkeley Common Source Stage λ =

More information

ANNOUNCEMENT ANNOUNCEMENT

ANNOUNCEMENT ANNOUNCEMENT ANNOUNCEMENT Exam : Tuesday September 25, 208, 8 PM - 0 PM Location: Elliott Hall of Music (see seating chart) Covers all readings, lectures, homework from Chapters 2 through 23 Multiple choice (5-8 questions)

More information

Systematic Circuit Analysis (T&R Chap 3)

Systematic Circuit Analysis (T&R Chap 3) Systematic Circuit Analysis (T&R Chap 3) Nodevoltage analysis Using the voltages of the each node relative to a ground node, write down a set of consistent linear equations for these voltages Solve this

More information

Active Circuits: Life gets interesting

Active Circuits: Life gets interesting Actie Circuits: Life gets interesting Actie cct elements operational amplifiers (P AMPS) and transistors Deices which can inject power into the cct External power supply normally comes from connection

More information

POLYTECHNIC UNIVERSITY Electrical Engineering Department. EE SOPHOMORE LABORATORY Experiment 2 DC circuits and network theorems

POLYTECHNIC UNIVERSITY Electrical Engineering Department. EE SOPHOMORE LABORATORY Experiment 2 DC circuits and network theorems POLYTECHNIC UNIVERSITY Electrical Engineering Department EE SOPHOMORE LABORATORY Experiment 2 DC circuits and network theorems Modified for Physics 18, Brooklyn College I. Overview of Experiment In this

More information

EE 581 Power Systems. Admittance Matrix: Development, Direct and Iterative solutions

EE 581 Power Systems. Admittance Matrix: Development, Direct and Iterative solutions EE 581 Power Systems Admittance Matrix: Development, Direct and Iterative solutions Overview and HW # 8 Chapter 2.4 Chapter 6.4 Chapter 6.1-6.3 Homework: Special Problem 1 and 2 (see handout) Overview

More information

A Small-Signal Analysis of a BJT

A Small-Signal Analysis of a BJT 3/28/2011 A mall ignal Analysis of a BJ lecture 1/12 A mall-ignal Analysis of a BJ he collector current i of a BJ is related to its base-emitter oltage as: i i e Jim tiles he Uni. of Kansas Dept. of EE

More information

Thevenin equivalent circuits

Thevenin equivalent circuits Thevenin equivalent circuits We have seen the idea of equivalency used in several instances already. 1 2 1 2 same as 1 2 same as 1 2 R 3 same as = 0 V same as 0 A same as same as = EE 201 Thevenin 1 The

More information

Physics 102: Lecture 06 Kirchhoff s Laws

Physics 102: Lecture 06 Kirchhoff s Laws Physics 102: Lecture 06 Kirchhoff s Laws Physics 102: Lecture 6, Slide 1 Today Last Lecture Last Time Resistors in series: R eq = R 1 R 2 R 3 Current through each is same; Voltage drop is IR i Resistors

More information

3.1 Superposition theorem

3.1 Superposition theorem Many electric circuits are complex, but it is an engineer s goal to reduce their complexity to analyze them easily. In the previous chapters, we have mastered the ability to solve networks containing independent

More information

EE 202L Linear Circuits. Class #1

EE 202L Linear Circuits. Class #1 EE 202L Linear Circuits Class #1 Course Personnel Prof. Edward Maby maby@usc.edu 0-4706 Office Hours: TTh 1:00-2:00 PHE 606 Dr. Douglas Burke burked@usc.edu 0-4711 Office Hours: TTh 12:30-2:00 PHE 430

More information