Operational Amplifiers

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

PHYS225 Lecture 9. Electronic Circuits

Lecture 4: Feedback and Op-Amps

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 =

Lecture 7: Transistors and Amplifiers

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

ECE2262 Electric Circuits. Chapter 4: Operational Amplifier (OP-AMP) Circuits

EE100Su08 Lecture #9 (July 16 th 2008)

E1.1 Analysis of Circuits ( ) Revision Lecture 1 1 / 13

DESIGN MICROELECTRONICS ELCT 703 (W17) LECTURE 3: OP-AMP CMOS CIRCUIT. Dr. Eman Azab Assistant Professor Office: C

ELECTRONIC SYSTEMS. Basic operational amplifier circuits. Electronic Systems - C3 13/05/ DDC Storey 1

EE 321 Analog Electronics, Fall 2013 Homework #3 solution

Lecture 5: Using electronics to make measurements

Georgia Institute of Technology School of Electrical and Computer Engineering. Midterm-1 Exam (Solution)

Final Exam. 55:041 Electronic Circuits. The University of Iowa. Fall 2013.

55:041 Electronic Circuits The University of Iowa Fall Final Exam

ESE319 Introduction to Microelectronics. Output Stages

Electronics II Physics 3620 / 6620

Homework Assignment 08

EE-201 Review Exam I. 1. The voltage Vx in the circuit below is: (1) 3V (2) 2V (3) -2V (4) 1V (5) -1V (6) None of above

Studio 9 Review Operational Amplifier Stability Compensation Miller Effect Phase Margin Unity Gain Frequency Slew Rate Limiting Reading: Text sec 5.

Electronic Circuits. Prof. Dr. Qiuting Huang Integrated Systems Laboratory

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

FEEDBACK AND STABILITY

ECE-343 Test 2: Mar 21, :00-8:00, Closed Book. Name : SOLUTION

ESE319 Introduction to Microelectronics Common Emitter BJT Amplifier

ENGR-4300 Spring 2009 Test 2. Name: SOLUTION. Section: 1(MR 8:00) 2(TF 2:00) 3(MR 6:00) (circle one) Question I (20 points): Question II (20 points):

E40M. Op Amps. M. Horowitz, J. Plummer, R. Howe 1


At point G V = = = = = = RB B B. IN RB f

Time Varying Circuit Analysis

Chapter 10 Feedback. PART C: Stability and Compensation

ECE Analog Integrated Circuit Design - II P.E. Allen

Feedback Control G 1+FG A

Electronics II. Final Examination

CARLETON UNIVERSITY. FINAL EXAMINATION December DURATION 3 HOURS No. of Students 130

Simultaneous equations for circuit analysis

Operational Amplifiers

CHAPTER.4: Transistor at low frequencies

Operational amplifiers (Op amps)

ECS 40, Fall 2008 Prof. Chang-Hasnain Test #3 Version A

OPERATIONAL AMPLIFIER APPLICATIONS

KOM2751 Analog Electronics :: Dr. Muharrem Mercimek :: YTU - Control and Automation Dept. 1 7 DC BIASING FETS (CONT D)

EE105 Fall 2014 Microelectronic Devices and Circuits

ESE319 Introduction to Microelectronics. Feedback Basics

Chapter 2. Engr228 Circuit Analysis. Dr Curtis Nelson

Lecture 5: Using electronics to make measurements

The BJT Differential Amplifier. Basic Circuit. DC Solution

Series & Parallel Resistors 3/17/2015 1

Chapter 2 - DC Biasing - BJTs

Physics 364, Fall 2012, reading due your answers to by 11pm on Thursday

Solved Problems. Electric Circuits & Components. 1-1 Write the KVL equation for the circuit shown.

Fundamentals of Electric Circuits, Second Edition - Alexander/Sadiku

Operational Amplifier (Op-Amp) Operational Amplifiers. OP-Amp: Components. Internal Design of LM741

Homework Assignment 09

OPAMPs I: The Ideal Case

Basic Electronics Prof. Dr. Chitralekha Mahanta Department of Electronics and Communication Engineering Indian Institute of Technology, Guwahati

mith College Computer Science CSC270 Spring 16 Circuits and Systems Lecture Notes Week 3 Dominique Thiébaut

or Op Amps for short

Homework 6 Solutions and Rubric

KOM2751 Analog Electronics :: Dr. Muharrem Mercimek :: YTU - Control and Automation Dept. 1 4 DC BIASING BJTS (CONT D II )

ECE-343 Test 1: Feb 10, :00-8:00pm, Closed Book. Name : SOLUTION

ECEN 325 Electronics

UNIT 4 DC EQUIVALENT CIRCUIT AND NETWORK THEOREMS

Section 1: Common Emitter CE Amplifier Design

HC5503PRC SLIC and the IDT Quad PCM CODEC with Programmable Gain

Feedback design for the Buck Converter

Problem Set 4 Solutions

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

Frequency Dependent Aspects of Op-amps

Electronic Circuits Summary

Electronics Prof. D C Dube Department of Physics Indian Institute of Technology Delhi

Texas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos

Sample-and-Holds David Johns and Ken Martin University of Toronto

BJT Biasing Cont. & Small Signal Model

ECE137B Final Exam. Wednesday 6/8/2016, 7:30-10:30PM.

Section 4. Nonlinear Circuits

Quick Review. ESE319 Introduction to Microelectronics. and Q1 = Q2, what is the value of V O-dm. If R C1 = R C2. s.t. R C1. Let Q1 = Q2 and R C1

Experiment 9 Equivalent Circuits

EE214 Early Final Examination: Fall STANFORD UNIVERSITY Department of Electrical Engineering. SAMPLE FINAL EXAMINATION Fall Quarter, 2002

Electrical System Elements

Operational amplifiers (Op amps)

Application Report. Mixed Signal Products SLOA021

Biasing BJTs CHAPTER OBJECTIVES 4.1 INTRODUCTION

Biasing the CE Amplifier

EE 321 Analog Electronics, Fall 2013 Homework #8 solution

ID # NAME. EE-255 EXAM 3 April 7, Instructor (circle one) Ogborn Lundstrom

Lecture 11: J-FET and MOSFET

Lecture 25 ANNOUNCEMENTS. Reminder: Prof. Liu s office hour is cancelled on Tuesday 12/4 OUTLINE. General considerations Benefits of negative feedback

The Approximating Impedance

Switched-Capacitor Circuits David Johns and Ken Martin University of Toronto

ECE 220 Laboratory 4 Volt Meter, Comparators, and Timer

Chapter 2. - DC Biasing - BJTs

ECE3050 Assignment 7

CHAPTER 3: TRANSISTOR MOSFET DR. PHAM NGUYEN THANH LOAN. Hà Nội, 9/24/2012

Lecture 13 MOSFET as an amplifier with an introduction to MOSFET small-signal model and small-signal schematics. Lena Peterson

D C Circuit Analysis and Network Theorems:

P1: Basics - Things you now know that you didn t know you knew (25 pts)

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

The Common-Emitter Amplifier

Transcription:

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 input impedance and zero output impedance. An integrated circuit (IC) contains a number of components on a single piece of semiconductor. Most op-amps are IC chips. 1

The 741 Operational Amplifier Op-Amp Input/Output We consider the opamp as a single component with input and output characteristics. Two signal inputs: Inverting Non-inverting Two dc power supply leads (+ and ) One output lead 2

Op-Amp Packages The Operation of Op-amps The input stage of an op-amp is a differential amplifier. The op-amp amplifies the difference between the two input terminal voltages. V diff =V 2 V 1 V 1 V 2 + 3

Op-Amp Output The output of the amplifier is determined by The gain of the amplifier. The polarity relationship between V 1 and V 2. The values of the supply voltages, +V and -V. The load resistance Op-Amp Gain The maximum possible gain of an op-amp is called the open-loop gain A OL. Generally A OL is greater than 10,000. Typical values are on the order of 200,000. An ideal op-amp would have infinite gain. 4

Input/Output Polarity The output polarity follows the sign of V diff. If V 2 V 1 > 0 the output polarity will be positive. If V 2 V 1 < 0 the output polarity will be negative. V 1 V 2 + Supply Voltages The supply voltages determine the limits of output voltage swing. No matter what the gain and input voltages the output value can not exceed +V or V. In practice the maximum output voltage is slightly less than the supply voltages. For resistive loads > 10kΩ the output voltages are about 1V less than the supply voltages. For resistive loads > 2kΩ the output voltages are about 2V less than the supply voltages. 5

Open Loop Op-amp Use As the open loop gain of most op-amps is extremely large the output of an open-loop circuit is either the maximum positive or negative voltage. +15 V V 1 V 2 + # + 14 V V > V 2 V out = " $ 14 V V2 <! V 1 1-15 V Feedback Circuits 6

Feedback Most op-amp circuits are designed to use feedback. Feedback is defined as taking a portion of the output of a circuit and coupling or feeding it back into the input. If the output fed back is in phase with the input then the circuit has positive feedback. If the output fed back is out of phase with the input then the circuit has negative feedback. Negative Feedback Most amplifiers use negative feedback. Disadvantages: decreased gain. Advantages: increased circuit stability, increased input impedance, decreased output impedance, increased frequency bandwidth at constant gain. 7

Negative Voltage Feedback A fraction B < 1 of the output voltage is subtracted from the input voltage. v " =! Bv out Σ v A OL v out -B Negative Voltage Feedback The closed loop gain, A v, is defined as The closed loop gain can be calculated from two equations Σ v A OL v out -B 8

Negative Voltage Feedback Solving for A v gives Usually the open-loop gain is so large that we can approximate: Σ v A OL v out -B Negative Feedback The gain of the amplifier circuit depends only on B, the fraction of output voltage fed back. B can be made very constant so that the amplifier has great gain stabilization. Bv out R 1 v out Example: B could be determined by two resistors in a voltage divider relationship. R 2 9

Negative Feedback Impedance The input and output impedance is also changed by the feedback. Op-Amp Circuits With Negative Feedback 10

Non-Inverting Amplifier Using Kirchoff s rule, Ohm s Law, and our knowledge of op-amps we can derive a closed loop-voltage gain for the non-inverting amplifier circuit shown below. i 2 i 1 R 2 R 1 i v 1 v 2 v out Non-Inverting Amplifier As the input resistance of the op-amp is very large we can neglect i. The output voltage is given by the voltage difference and the open-loop gain. i 2 i 1 R 2 R 1 i v 1 v 2 v out 11

Non-Inverting Amplifier Combining the previous equations we find: A v = v out = A OL (R 1 + R 2 ) (A OL +1)R 1 + R 2 If the open-loop gain is very large: i 2 i 1 R 2 R 1 i v 1 v 2 v out Inverting Amplifier Using Kirchoff s rule, Ohm s Law, and our knowledge of op-amps we can derive a closed loop-voltage gain for the inverting amplifier circuit shown below i 2 i 1 R 2 R 1 i v 1 v 2 vout 12

Inverting Amplifier The output voltage is related to the voltage difference. Neglecting i and combining the equations gives i 2 i 1 R 2 R 1 i v 1 v 2 vout Inverting Amplifier For a very large open-loop gain becomes i 2 i 1 R 2 R 1 i v 1 v 2 vout 13

The Two Golden Rules of Op-Amp Circuits Notice in both derivations two approximations were made: (1) the input current i flowing into the op-amp was neglected compared to other currents; and (2) the open-loop op amp gain A OL was assumed to be very large compared to the gain with feedback. These two approximations can be extended to form two golden rules for analyzing an op-amp circuits with negative feedback. Op-Amp Current Rule (OACR): The current into or out of each op-amp input terminal is approximately zero. Op-Amp Voltage Rule (OAVR): The voltage difference between the two op-amp input terminals is approximately zero. Op-Amp Current Rule The OACR basically says that the input impedance of the op-amp is much higher than the external input impedance from the input terminal to ground. For BJT op-amps input impedance is on the order of 10MΩ. For FET op-amps input impedance is on the order of 10 12 Ω. 14

Op-Amp Voltage Rule The OAVR is the equivalent of saying that the open-loop gain is infinite. The output of the op-amp can never be greater than the supply voltage (~15V) which means that (v 2 -v 1 ) must be less that 150 µv for a typical A OL or the output will be saturated. Therefore if the op-amp is not saturated then the difference between the input terminals must be nearly zero. The rule says that in an actual op amp circuit the negative feedback plus the high gain of the op-amp effectively zeros the difference between the two inputs. Non-inverting Amp OACR: i 1 = i 2 OAVR: v 1 = v 2 = i 2 i R 1 2 R 1 v 1 v 2 v out 15

Inverting Amp OACR: i 1 = i 2 OAVR: v 1 = v 2 = 0 i 2 i R 1 2 R 1 v 1 v 2 vout Instrumentation Amplifier 16

Peak Detection Amplifier Positive Feedback 17

Positive Feedback Circuits Rather than placing a portion of the output back into the inverting input a portion of the output is sent back to the non-inverting terminal to produce positive feedback. Positive Feedback Circuits Oscillators 18

Positive Feedback Circuits Oscillators 19