ANALYSIS OF TRANSISTOR FEEDBACK AMPLIFIERS
|
|
- Tamsyn Jefferson
- 6 years ago
- Views:
Transcription
1 ECE 3050 Analysis of s Page 1 ANALYSS F TANSST FEEDBACK AMPLFES Steps n Analyzing s 1. dentify the topology. 2. Determine whether the is positive negative. 3. pen the loop and calculate A, ß,, and o. 4. se the Table to find A f, f and of A F, F, and of. 5. se the infmation in 4.) to find whatever is required (ut /n, n, out, etc.) Generic Concept Properties of a Generic A signal can only go out the terminal A signal can only go in the terminal A signal can in out the terminal dentification of the Topology solate the input and output transist(s) and apply the following identification. nput Series: v s Shunt: utput Series: L Shunt: L L L
2 ECE 3050 Analysis of s Page 2 EXAMPLE F FEEDBACK TPLGY DENTFCATN se the rules of identifying topologies to identify the four different topologies f the circuits shown below. Circuits 1 and 2 5V M3 M4 V in M1 M2 M5 M6 V out1 V out2 M7 5V Circuits 3 and 4 5V M3 M4 M5 V out1 V in M1 M2 M6 V out2 M7 5V
3 ECE 3050 Analysis of s Page 3 LES F DENTFYNG PSTVE AND NEGATVE FEEDBACK 1. dentify the loop by tracing its path on the diagram. f there are alternate paths, always choose the path with the highest loop gain. (emember that a signal can go in the "" "" terminal of a transist and can only come out the "" "" terminal.) 2. At any point on the loop, assume the signal is positive and put a "" mark at that point. Trace the signal around the loop remembering that the signal only inverts when it goes in a "" terminal and out the "" terminal of a transist. All other paths through a transist do not invert (i.e., "" to "" and "" to ""). 3. When you have traced the polarity of the signal around the loop back to the point where you placed the "", the is negative if the signal polarity is "" and positive if the signal polarity is "". Example Example 2 5V V in M3 M4 M5 M1 M2 M6 V out1 V out2 M7 5V
4 ECE 3050 Analysis of s Page 4 EXAMPLE F FEEDBACK TPLGY DENTFCATN se the rules of identifying topologies to create the four different negative topologies using the identical starting structure. 1. VoltageVoltage (SeriesShunt) 2. CurrentVoltage (ShuntShunt) VoltageCurrent (SeriesSeries) 4. CurrentCurrent (ShuntSeries)
5 ECE 3050 Analysis of s Page 5 LES F ANALYSS F TANSST FEEDBACK AMPLFES SeriesShunt nput nput est of utput utput = esistance seen looking out the terminal of the input transist with = 0. = esistance seen looking out the terminal of the output transist with = 0. SeriesSeries nput est of utput utput = esistance seen looking out the terminal of the input transist with = 0. = esistance seen looking out the terminal of the output transist with = 0. ShuntShunt nput est of nput nput utput utput = esistance seen looking out the terminal of the input transist with = 0. = esistance seen looking out the terminal of the output transist with = 0. ShuntSeries nput utput nput est of utput = esistance seen looking out the terminal of the input transist with = 0. = esistance seen looking out the terminal of the output transist with = 0.
6 ECE 3050 Analysis of s Page 6 Summary of the mptant elationships of penloop and Closedloop s. Quantity nputoutput variable Voltage Transconductance Transresistance Current Voltagevoltage Voltagecurrent Currentvoltage Currentcurrent Small Signal Model A vf n o o o Gmf n mf n Aif n o Small Signal S with o S o io S Source & Load L A vf v ol S o io i G mf L mf i A if L deal S S = 0 S << S = 0 S << S = S >> S = S >> deal L L = L >> o L = 0 L << o L = L >> o L = 0 L << o verall Fward L A vf o G mf S L mf S o A if Gain AV= GM= M= ( S )( L o ) ( S i)( L o ) ( S i)( L o ) A = ( S i)( L o ) Topology Seriesshunt Seriesseries Shuntshunt Shuntseries deal ß, finite F F F S and L T F F i F o o Small i v S o o s βv L o A Signal Models vf v i L v s o β L L F S β i G mf v mf i S βio i Aif T F ClosedLoop Gain (deal S and L ) ClosedLoop nput esistance (deal S and L ) ClosedLoop utput esistance (deal S and L ) ClosedLoop Gain ClosedLoop nput esistance ClosedLoop utput esistance utput esistance of Series utput Fb. Ckt A vf = Avf (1A vf ß v ) G mf = Gmf (1G mf ß g ) F = (1 A vf ß v ) F = (1 G mf ß g ) of = A VF = o of = o (1 mf ß g ) 1 A vf ß v AV (1A V ß v ) F = ( S )(1A V ß v ) F = o L o L 1 A V ßv T = F G MF = GM (1G M ß g ) mf = F = of = F = ( S )(1 G M ß g ) F = mf (1 mf ß r ) A if = Aif (1A if ß i ) 1 mf ß if = r 1 A if ß i o of = o (1 A if ß i ) 1 mf ß r M MF = (1 M ß r ) S o L F = o L ( o L )(1G M ß g ) F = 1 M ßr S 1 M ß r F = A A F = (1A ß i ) S S 1 A ß i F = ( o L )(1A ß i ) T = L F ( F L ) T = F T = L F ( F L )
Lectures on FEEDBACK FB-1. Feedback. Analog Circuit Design FB-5 FB-2. Feedback (Cont.) Feedback (Cont.) There are 4 basic kinds of Feedback Circuits :
bert W. Brdersen EECS40 University f Clifrni Berkeley Cllege f Engeerg Deprtment f Electricl Engeerg nd Cmputer Science Anlg Circuit Design Lectures n FEEDBACK Feedbck Σ Errr Signl Feedbck Signl fb Bsic
More informationFeedback and Oscillator Circuits
and Oscillator Circuits The input signal, Vs, is applied to a mixer network Here it is combined with a feedback signal V f Difference (or sum) of signals, V i, is then the input voltage to the amplifier
More informationFeedback Principle :-
Feedback Prncple : Feedback amplfer s that n whch a part f the utput f the basc amplfer s returned back t the nput termnal and mxed up wth the nternal nput sgnal. The sub netwrks f feedback amplfer are:
More informationc Copyright 2009. W. Marshall Leach, Jr., Professor, Georgia Institute of Technology, School of Electrical and Computer Engineering. Feedback Amplifiers CollectionofSolvedProblems A collection of solved
More informationLecture 7: Two-Ports (2)
Lecture 7: Two-Ports (2) Amin Arbabian Jan M. Rabaey EE142 Fall 2010 Sept. 16 th, 2010 Announcements HW3 Posted, due Thursday September 23 rd, 330pm EE142 drop box. Office hours Two-Port notes by Professor
More informationFeedback Transimpedance & Current Amplifiers
Feedback Transimpedance & Current Amplifiers Willy Sansen KULeuven, ESATMICAS Leuven, Belgium willy.sansen@esat.kuleuven.be Willy Sansen 1005 141 Table of contents Introduction Shuntshunt FB for Transimpedance
More informationECE Analog Integrated Circuit Design - II P.E. Allen
Lecture 290 Feedback Analysis using Return Ratio (3/20/02) Page 2901 LECTURE 290 FEEDBACK CIRCUIT ANALYSIS USING RETURN RATIO (READING: GHLM 599613) Objective The objective of this presentation is: 1.)
More information320-amp-models.tex Page 1 ECE 320. Amplifier Models. ECE Linear Active Circuit Design
320ampmodels.tex Page 1 ECE 320 Amplifier Models ECE 320 Linear Active Circuit Design 320ampmodels.tex Page 2 2Port Networks A 2port network is any circiut with two pairs of wires connecting to the outside
More informationElectronics II. Midterm #2
The University of Toledo EECS:3400 Electronics I su4ms_elct7.fm Section Electronics II Midterm # Problems Points. 8. 7 3. 5 Total 0 Was the exam fair? yes no The University of Toledo su4ms_elct7.fm Problem
More informationECE 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 informationor Op Amps for short
or Op Amps for short Objective of Lecture Describe how an ideal operational amplifier (op amp) behaves. Define voltage gain, current gain, transresistance gain, and transconductance gain. Explain the operation
More informationECE321 Electronics I
ECE31 Electronics Lecture 1: CMOS nverter: Noise Margin & Delay Model Payman Zarkesh-Ha Office: ECE Bldg. 30B Office hours: Tuesday :00-3:00PM or by appointment E-mail: payman@ece.unm.edu Slide: 1 CMOS
More informationElectronics 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 informationOperational Amplifiers
Operational Amplifiers A Linear IC circuit Operational Amplifier (op-amp) An op-amp is a high-gain amplifier that has high input impedance and low output impedance. An ideal op-amp has infinite gain and
More informationLecture 7: Transistors and Amplifiers
Lecture 7: Transistors and Amplifiers Hybrid Transistor Model for small AC : The previous model for a transistor used one parameter (β, the current gain) to describe the transistor. doesn't explain many
More informationECE2262 Electric Circuits. Chapter 4: Operational Amplifier (OP-AMP) Circuits
ECE2262 Electric Circuits Chapter 4: Operational Amplifier (OP-AMP) Circuits 1 4.1 Operational Amplifiers 2 4. Voltages and currents in electrical circuits may represent signals and circuits can perform
More informationLesson #14. Section BME 373 Electronics II J.Schesser
Feedback and Oscillatrs Lessn #4 Impedances Sectin 9.35 65 Types f ffeedback Type f ffeedback k(the utput tentity fed dback): Vltage Feedback s. Current Feedback β s. β Hw it is achieed (the means t fed
More information1. 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 informationTransistors. Lesson #10 Chapter 4. BME 372 Electronics I J.Schesser
Tanssts essn #10 Chapte 4 BM 372 lectncs 154 Hmewk Ps. 4.40, 4.42, 4.43, 4.45, 4.46, 4.51, 4.53, 4.54, 4.56 BM 372 lectncs 155 Hmewk Answes #20 Ps. 4.40 See fgue 4.33 BM 372 lectncs 156 Ps. 4.42 Hmewk
More informationAnalog Circuits and Systems
Analog Circuits and Systems Prof. K Radhakrishna Rao Lecture 5 Analog Signal Processing using One Port Networks, Passive Two Ports and Ideal Amplifiers 1 One Port Devices Passive devices like R, L, C and
More information55:141 Advanced Circuit Techniques Two-Port Theory
55:4 Adanced Crcut Technques Two-Port Theory Materal: Lecture Notes A. Kruger 55:4: Adanced Crcut Technques The Unersty of Iowa, 03 Two-Port Theory, Slde What Are Two-Ports? Basc dea: replace a complex
More informationReview 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 informationElectronics II. Midterm #2
The University of Toledo EECS:3400 Electronics I Section sums_elct7.fm - StudentName Electronics II Midterm # Problems Points. 8. 3. 7 Total 0 Was the exam fair? yes no The University of Toledo sums_elct7.fm
More informationExact Analysis of a Common-Source MOSFET Amplifier
Exact Analysis of a Common-Source MOSFET Amplifier Consider the common-source MOSFET amplifier driven from signal source v s with Thévenin equivalent resistance R S and a load consisting of a parallel
More informationTwo Port Characterizations
lectronc Crcuts Two Port Characterzatons Contents Input and output resstances Two port networks Models Prof. C.K. Tse: -port networks Impedances and loadng effects Voltage amplfers R s R out smaller the
More informationDepartment of Electrical and Computer Engineering FEEDBACK AMPLIFIERS
Department o Electrcal and Computer Engneerng UNIT I EII FEEDBCK MPLIFIES porton the output sgnal s ed back to the nput o the ampler s called Feedback mpler. Feedback Concept: block dagram o an ampler
More informationThe equivalent model of a certain op amp is shown in the figure given below, where R 1 = 2.8 MΩ, R 2 = 39 Ω, and A =
The equivalent model of a certain op amp is shown in the figure given below, where R 1 = 2.8 MΩ, R 2 = 39 Ω, and A = 10 10 4. Section Break Difficulty: Easy Learning Objective: Understand how real operational
More informationOperational amplifiers (Op amps)
Operational amplifiers (Op amps) v R o R i v i Av i v View it as an ideal amp. Take the properties to the extreme: R i, R o 0, A.?!?!?!?! v v i Av i v A Consequences: No voltage dividers at input or output.
More informationECE 3050A, Spring 2004 Page 1. FINAL EXAMINATION - SOLUTIONS (Average score = 78/100) R 2 = R 1 =
ECE 3050A, Spring 2004 Page Problem (20 points This problem must be attempted) The simplified schematic of a feedback amplifier is shown. Assume that all transistors are matched and g m ma/v and r ds.
More informationLecture 17 Date:
Lecture 17 Date: 27.10.2016 Feedback and Properties, Types of Feedback Amplifier Stability Gain and Phase Margin Modification Elements of Feedback System: (a) The feed forward amplifier [H(s)] ; (b) A
More informationMicroelectronic Circuit Design 4th Edition Errata - Updated 4/4/14
Chapter Text # Inside back cover: Triode region equation should not be squared! i D = K n v GS "V TN " v & DS % ( v DS $ 2 ' Page 49, first exercise, second answer: -1.35 x 10 6 cm/s Page 58, last exercise,
More informationOPERATIONAL AMPLIFIER APPLICATIONS
OPERATIONAL AMPLIFIER APPLICATIONS 2.1 The Ideal Op Amp (Chapter 2.1) Amplifier Applications 2.2 The Inverting Configuration (Chapter 2.2) 2.3 The Non-inverting Configuration (Chapter 2.3) 2.4 Difference
More informationECS 40, Fall 2008 Prof. Chang-Hasnain Test #3 Version A
ECS 40, Fall 2008 Prof. ChangHasnain Test #3 Version A 10:10 am 11:00 am, Wednesday December 3, 2008 Total Time Allotted: 50 minutes Total Points: 100 1. This is a closed book exam. However, you are allowed
More informationOperational amplifiers (Op amps)
Operational amplifiers (Op amps) Recall the basic two-port model for an amplifier. It has three components: input resistance, Ri, output resistance, Ro, and the voltage gain, A. v R o R i v d Av d v Also
More information1/13/12 V DS. I d V GS. C ox ( = f (V GS ,V DS ,V SB = I D. + i d + I ΔV + I ΔV BS V BS. 19 January 2012
/3/ 9 January 0 Study the linear model of MOS transistor around an operating point." MOS in saturation: V GS >V th and V S >V GS -V th " VGS vi - I d = I i d VS I d = µ n ( L V V γ Φ V Φ GS th0 F SB F
More informationGoals for today 2.004
Goals for today Block diagrams revisited Block diagram components Block diagram cascade Summing and pickoff junctions Feedback topology Negative vs positive feedback Example of a system with feedback Derivation
More informationCURRENT SOURCES EXAMPLE 1 Find the source voltage Vs and the current I1 for the circuit shown below SOURCE CONVERSIONS
CURRENT SOURCES EXAMPLE 1 Find the source voltage Vs and the current I1 for the circuit shown below EXAMPLE 2 Find the source voltage Vs and the current I1 for the circuit shown below SOURCE CONVERSIONS
More informationECE 342 Electronic Circuits. Lecture 25 Frequency Response of CG, CB,SF and EF
ECE 342 Electronic Circuits ecture 25 Frequency esponse of CG, CB,SF and EF Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jesa@illinois.edu ECE 342 Jose Schutt Aine 1 Common
More informationE40M. Op Amps. M. Horowitz, J. Plummer, R. Howe 1
E40M Op Amps M. Horowitz, J. Plummer, R. Howe 1 Reading A&L: Chapter 15, pp. 863-866. Reader, Chapter 8 Noninverting Amp http://www.electronics-tutorials.ws/opamp/opamp_3.html Inverting Amp http://www.electronics-tutorials.ws/opamp/opamp_2.html
More information55:141 Advanced Circuit Techniques Two-Port Theory
55:4 Adanced Crcut Technques Two-Port Theory Materal: Lecture Notes A. Kruger 55:4: Adanced Crcut Technques The Unersty of Iowa, 205 Two-Port Theory, Slde Two-Port Networks Note, the BJT s all are hghly
More informationPower Management Circuits and Systems. Basic Concepts: Amplifiers and Feedback. Jose Silva-Martinez
Power Management Circuits and Systems Basic Concepts: Amplifiers and Feedback Jose Silva-Martinez Department of Electrical & Computer Engineering Texas A&M University January 2, 209 Non-Inverting Amplifier
More informationECE 6412, Spring Final Exam Page 1
ECE 64, Spring 005 Final Exam Page FINAL EXAMINATION SOLUTIONS (Average score = 89/00) Problem (0 points This problem is required) A comparator consists of an amplifier cascaded with a latch as shown below.
More informationTaking the Laplace transform of the both sides and assuming that all initial conditions are zero,
The transfer function Let s begin with a general nth-order, linear, time-invariant differential equation, d n a n dt nc(t)... a d dt c(t) a 0c(t) d m = b m dt mr(t)... a d dt r(t) b 0r(t) () where c(t)
More informationUNIVERSITÀ DEGLI STUDI DI CATANIA. Dottorato di Ricerca in Ingegneria Elettronica, Automatica e del Controllo di Sistemi Complessi, XXII ciclo
UNIVERSITÀ DEGLI STUDI DI CATANIA DIPARTIMENTO DI INGEGNERIA ELETTRICA, ELETTRONICA E DEI SISTEMI Dottorato di Ricerca in Ingegneria Elettronica, Automatica e del Controllo di Sistemi Complessi, XXII ciclo
More informationRIB. ELECTRICAL ENGINEERING Analog Electronics. 8 Electrical Engineering RIB-R T7. Detailed Explanations. Rank Improvement Batch ANSWERS.
8 Electrical Engineering RIB-R T7 Session 08-9 S.No. : 9078_LS RIB Rank Improvement Batch ELECTRICL ENGINEERING nalog Electronics NSWERS. (d) 7. (a) 3. (c) 9. (a) 5. (d). (d) 8. (c) 4. (c) 0. (c) 6. (b)
More informationPHYS225 Lecture 9. Electronic Circuits
PHYS225 Lecture 9 Electronic Circuits Last lecture Field Effect Transistors Voltage controlled resistor Various FET circuits Switch Source follower Current source Similar to BJT Draws no input current
More informationSPS Presents: A Cosmic Lunch!
SPS Presents: A Cosmic Lunch! Who: Dr. Brown will be speaking about Evolution of the Elements: from Periodic table to Standard Model and Beyond! When: October 7 th at am Where: CP 79 (by the front office)
More informationEE105 Fall 2014 Microelectronic Devices and Circuits
EE05 Fall 204 Microelectronic Devices and Circuits Prof. Ming C. Wu wu@eecs.berkeley.edu 5 Sutardja Dai Hall (SDH) Terminal Gain and I/O Resistances of BJT Amplifiers Emitter (CE) Collector (CC) Base (CB)
More informationElectronics II. Midterm #1
The University of Toledo EECS:3400 Electronics I su3ms_elct7.fm Section Electronics II Midterm # Problems Points. 5. 6 3. 9 Total 0 Was the exam fair? yes no The University of Toledo su3ms_elct7.fm Problem
More informationUnderstanding Loading in Feedback Amplifier Analysis
Understanding Loading in Feedback Amplifier Analysis Manuel ToledoQuiñones Electrical and Computer Engineering Department University of Puerto Rico Mayagüez, Puerto Rico Session 1532 Introduction The application
More informationECE2262 Electric Circuits
ECE2262 Electric Circuits Equivalence Chapter 5: Circuit Theorems Linearity Superposition Thevenin s and Norton s Theorems Maximum Power Transfer Analysis of Circuits Using Circuit Theorems 1 5. 1 Equivalence
More informationANNOUNCEMENT 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 informationFinal Exam. 55:041 Electronic Circuits. The University of Iowa. Fall 2013.
Final Exam Name: Max: 130 Points Question 1 In the circuit shown, the op-amp is ideal, except for an input bias current I b = 1 na. Further, R F = 10K, R 1 = 100 Ω and C = 1 μf. The switch is opened at
More informationMAE140 - 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 informationLECTURE 12 Lossy Converters (Static State Losses but Neglecting Switching Losses) HW #2 Erickson Chapter 3 Problems 6 & 7 A.
ETUE 12 ossy onverters (Static State osses but Neglecting Switching osses) HW #2 Erickson hapter 3 Problems 6 & 7 A. General Effects Expected: (load) as (load) B. Switch and esistive osses hange M(D) Modified
More informationOPAMPs I: The Ideal Case
I: The Ideal Case The basic composition of an operational amplifier (OPAMP) includes a high gain differential amplifier, followed by a second high gain amplifier, followed by a unity gain, low impedance,
More informationSWITCHED CAPACITOR AMPLIFIERS
SWITCHED CAPACITOR AMPLIFIERS AO 0V 4. AO 0V 4.2 i Q AO 0V 4.3 Q AO 0V 4.4 Q i AO 0V 4.5 AO 0V 4.6 i Q AO 0V 4.7 Q AO 0V 4.8 i Q AO 0V 4.9 Simple amplifier First approach: A 0 = infinite. C : V C = V s
More informationBrian Blais Quick Homemade Guide to Circuits
Brian Blais Quick Homemade Guide to Circuits 1 Initial Equations and Concepts Current, I. Units:amps rate of flow of charge: I = Q/ t Potential difference, V. Units: volts esistance,. Units:ohms Ohm s
More informationEE100Su08 Lecture #9 (July 16 th 2008)
EE100Su08 Lecture #9 (July 16 th 2008) Outline HW #1s and Midterm #1 returned today Midterm #1 notes HW #1 and Midterm #1 regrade deadline: Wednesday, July 23 rd 2008, 5:00 pm PST. Procedure: HW #1: Bart
More informationEIT Review. Electrical Circuits DC Circuits. Lecturer: Russ Tatro. Presented by Tau Beta Pi The Engineering Honor Society 10/3/2006 1
EIT Review Electrical Circuits DC Circuits Lecturer: Russ Tatro Presented by Tau Beta Pi The Engineering Honor Society 10/3/2006 1 Session Outline Basic Concepts Basic Laws Methods of Analysis Circuit
More informationHomework 6 Solutions and Rubric
Homework 6 Solutions and Rubric EE 140/40A 1. K-W Tube Amplifier b) Load Resistor e) Common-cathode a) Input Diff Pair f) Cathode-Follower h) Positive Feedback c) Tail Resistor g) Cc d) Av,cm = 1/ Figure
More information55:041 Electronic Circuits The University of Iowa Fall Final Exam
Final Exam Name: Score Max: 135 Question 1 (1 point unless otherwise noted) a. What is the maximum theoretical efficiency for a class-b amplifier? Answer: 78% b. The abbreviation/term ESR is often encountered
More informationECE2262 Electric Circuits. Chapter 5: Circuit Theorems
ECE2262 Electric Circuits Chapter 5: Circuit Theorems 1 Equivalence Linearity Superposition Thevenin s and Norton s Theorems Maximum Power Transfer Analysis of Circuits Using Circuit Theorems 2 5. 1 Equivalence
More information55:041 Electronic Circuits
55:04 Electronc Crcuts Feedback & Stablty Sectons of Chapter 2. Kruger Feedback & Stablty Confguraton of Feedback mplfer Negate feedback β s the feedback transfer functon S o S S o o S S o f S S S S fb
More informationESE319 Introduction to Microelectronics. Feedback Basics
Feedback Basics Feedback concept Feedback in emitter follower Stability One-pole feedback and root locus Frequency dependent feedback and root locus Gain and phase margins Conditions for closed loop stability
More informationCircuits. PHY2054: Chapter 18 1
Circuits PHY2054: Chapter 18 1 What You Already Know Microscopic nature of current Drift speed and current Ohm s law Resistivity Calculating resistance from resistivity Power in electric circuits PHY2054:
More informationEE 321 Analog Electronics, Fall 2013 Homework #8 solution
EE 321 Analog Electronics, Fall 2013 Homework #8 solution 5.110. The following table summarizes some of the basic attributes of a number of BJTs of different types, operating as amplifiers under various
More informationR R V I R. Conventional Current. Ohms Law V = IR
DC Circuits opics EMF and erminal oltage esistors in Series and in Parallel Kirchhoff s ules EMFs in Series and in Parallel Capacitors in Series and in Parallel Ammeters and oltmeters Conventional Current
More informationFeedback in Electronic Circuits
ROCHESTER INSTITUTE OF TECHNOLOGY MICROELECTRONIC ENGINEERING Feedback in Electronic Circuits Dr. Lynn Fuller Webpage: http://people.rit.edu/lffeee/ 82 Lomb Memorial Drive Rochester, NY 146235604 Tel (585)
More informationDESIGN MICROELECTRONICS ELCT 703 (W17) LECTURE 3: OP-AMP CMOS CIRCUIT. Dr. Eman Azab Assistant Professor Office: C
MICROELECTRONICS ELCT 703 (W17) LECTURE 3: OP-AMP CMOS CIRCUIT DESIGN Dr. Eman Azab Assistant Professor Office: C3.315 E-mail: eman.azab@guc.edu.eg 1 TWO STAGE CMOS OP-AMP It consists of two stages: First
More informationFeedback Control G 1+FG A
Introduction to Operational Amplifiers Circuit Functionality So far, only passive circuits (C, L and LC) have been analyzed in terms of the time-domain operator T and the frequency-domain operator A(ω),
More informationT-model: - + v o. v i. i o. v e. R i
T-mdel: e gm - V Rc e e e gme R R R 23 e e e gme R R The s/c tanscnductance: G m e m g gm e 0 The nput esstance: R e e e e The utput esstance: R R 0 /c unladed ltage gan, R a g R m e gmr e 0 m e g me e/e
More informationSection 4. Nonlinear Circuits
Section 4 Nonlinear Circuits 1 ) Voltage Comparators V P < V N : V o = V ol V P > V N : V o = V oh One bit A/D converter, Practical gain : 10 3 10 6 V OH and V OL should be far apart enough Response Time:
More informationIntroduction of Two Port Network Negative Feedback (Uni lateral Case) Feedback Topology Analysis of feedback applications
Lectue Feedback mple ntductn w Pt Netwk Negatve Feedback Un lateal Case Feedback plg nalss eedback applcatns Clse Lp Gan nput/output esstances e:83h 3 Feedback w-pt Netwk z-paametes Open-Ccut mpedance
More informationGeorgia Institute of Technology School of Electrical and Computer Engineering. Midterm-1 Exam (Solution)
Georgia Institute of Technology School of Electrical and Computer Engineering Midterm-1 Exam (Solution) ECE-6414 Spring 2012 Friday, Feb. 17, 2012 Duration: 50min First name Solutions Last name Solutions
More informationCopyright Paul Tobin 63
DT, Kevin t. lectric Circuit Thery DT87/ Tw-Prt netwrk parameters ummary We have seen previusly that a tw-prt netwrk has a pair f input terminals and a pair f utput terminals figure. These circuits were
More informationKonstruktion av Vippor och Latchar
Konstruktion av Vippor och Latchar Datorarkitektur 1 (1DT038) Fördjupning November 2009 karl.marklund@it.uu.se Om du läser IT (1DT038) är detta material överkurs du bör dock redan vara bekant med hur det
More informationPower lines. Why do birds sitting on a high-voltage power line survive?
Power lines At large distances, the resistance of power lines becomes significant. To transmit maximum power, is it better to transmit high V, low I or high I, low V? (a) high V, low I (b) low V, high
More informationSeries & 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 informationDepartment of Electrical and Computer Engineering, Cornell University. ECE 3150: Microelectronics. Spring Exam 1 ` March 22, 2018
Department of Electrical and Computer Engineering, Cornell University ECE 3150: Microelectronics Spring 2018 Exam 1 ` March 22, 2018 INSTRUCTIONS: Every problem must be done in the separate booklet Only
More informationCHAPTER.4: Transistor at low frequencies
CHAPTER.4: Transistor at low frequencies Introduction Amplification in the AC domain BJT transistor modeling The re Transistor Model The Hybrid equivalent Model Introduction There are three models commonly
More informationInput and Output Impedances with Feedback
EE 3 Lecture Basic Feedback Configurations Generalized Feedback Schemes Integrators Differentiators First-order active filters Second-order active filters Review from Last Time Input and Output Impedances
More informationU1 is zero based because its noninverting terminal is connected to circuit common. Therefore, the circuit reference voltage is 0 V.
When you have completed this exercise, you will be able to operate a zener-clamped op amp comparator circuit using dc and ac voltages. You will verify your results with an oscilloscope. U1 is zero based
More information) Rotate L by 120 clockwise to obtain in!! anywhere between load and generator: rotation by 2d in clockwise direction. d=distance from the load to the
3.1 Smith Chart Construction: Start with polar representation of. L ; in on lossless lines related by simple phase change ) Idea: polar plot going from L to in involves simple rotation. in jj 1 ) circle
More informationLecture 2 Feedback Amplifier
Lectue Feedback mple ntductn w-pt Netwk Negatve Feedback Un-lateal Case Feedback plg nalss eedback applcatns Clse-Lp Gan nput/output esstances e:83hkn 3 Feedback mples w-pt Netwk z-paametes Open-Ccut mpedance
More informationBipolar Junction Transistor (BJT) - Introduction
Bipolar Junction Transistor (BJT) - Introduction It was found in 1948 at the Bell Telephone Laboratories. It is a three terminal device and has three semiconductor regions. It can be used in signal amplification
More informationChapter 3. FET Amplifiers. Spring th Semester Mechatronics SZABIST, Karachi. Course Support
Chapter 3 Spring 2012 4 th Semester Mechatronics SZABIST, Karachi 2 Course Support humera.rafique@szabist.edu.pk Office: 100 Campus (404) Official: ZABdesk https://sites.google.com/site/zabistmechatronics/home/spring-2012/ecd
More informationDesigning 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 informationANALOG ELECTRONICS DR NORLAILI MOHD NOH
24 ANALOG LTRONIS lass 5&6&7&8&9 DR NORLAILI MOHD NOH 3.3.3 n-ase cnfguatn V V Rc I π π g g R V /p sgnal appled t. O/p taken f. ted t ac gnd. The hybd-π del pdes an accuate epesentatn f the sall-sgnal
More informationEE 435. Lecture 2: Basic Op Amp Design. - Single Stage Low Gain Op Amps
EE 435 ecture 2: Basic Op Amp Design - Single Stage ow Gain Op Amps 1 Review from last lecture: How does an amplifier differ from an operational amplifier?? Op Amp Amplifier Amplifier used in open-loop
More informationGeneral Amplifiers. Analog Electronics Circuits Nagamani A N. Lecturer, PESIT, Bangalore 85. Cascade connection - FET & BJT
Analg lectrnics Circuits Nagamani A N Lecturer, PST, Bangalre 85 mail nagamani@pes.edu General Amplifiers Cascade cnnectin - FT & BJT Numerical Cascde cnnectin arlingtn cnnectin Packaged arlingtn cnnectin
More informationChapter 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 informationAs light level increases, resistance decreases. As temperature increases, resistance decreases. Voltage across capacitor increases with time LDR
LDR As light level increases, resistance decreases thermistor As temperature increases, resistance decreases capacitor Voltage across capacitor increases with time Potential divider basics: R 1 1. Both
More informationEE40 Lec 20. MOS Circuits
EE40 Lec 20 MOS Circuits eading: Chap. 12 of Hambley Supplement reading on MOS Circuits http://www.inst.eecs.berkeley.edu/~ee40/fa09/handouts/ee40_mos_circuit.pdf Slide 1 Bias circuits OUTLINE Smallsignal
More informationLecture 13 MOSFET as an amplifier with an introduction to MOSFET small-signal model and small-signal schematics. Lena Peterson
Lecture 13 MOSFET as an amplifier with an introduction to MOSFET small-signal model and small-signal schematics Lena Peterson 2015-10-13 Outline (1) Why is the CMOS inverter gain not infinite? Large-signal
More informationDirect Current (DC) Circuits
Direct Current (DC) Circuits NOTE: There are short answer analysis questions in the Participation section the informal lab report. emember to include these answers in your lab notebook as they will be
More informationECE 342 Electronic Circuits. Lecture 35 CMOS Delay Model
ECE 34 Electronic Circuits Lecture 35 CMOS Delay Model Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jesa@illinois.edu ECE 34 Jose Schutt Aine 1 Digital Circuits V IH : Input
More informationELG4125: Power Transmission Lines Steady State Operation
ELG4125: Power Transmission Lines Steady State Operation Two-Port Networks and ABCD Models A transmission line can be represented by a two-port network, that is a network that can be isolated from the
More informationLecture 120 Compensation of Op Amps-I (1/30/02) Page ECE Analog Integrated Circuit Design - II P.E. Allen
Lecture 20 Compensation of Op AmpsI (/30/02) Page 20 LECTURE 20 COMPENSATION OF OP AMPS I (READING: GHLM 425434 and 624638, AH 249260) INTRODUCTION The objective of this presentation is to present the
More informationAnalog Design Challenges in below 65nm CMOS
Analog Design Challenges in below 65nm CMOS T. R. Viswanathan University of Texas at Austin 4/11/2014 Seminar 1 Graduate Students Amit Gupta (TI):Two-Step VCO based ADC K. R. Raghunandan (Si Labs): Analog
More information