Inverting Amplifier Under stable linear operation – A OL = ∞, R in = ∞ – V o = A OL (V in(+) – V in(-) ) – V id = (V in(+) – V in(-) ) = V o /A OL = 0.

Slides:



Advertisements
Similar presentations
Introduction Goal: Understand the design of op-amp based ICs (comparators, oscillators, integrators, differentiators, instrumentation amplifiers) for applications.
Advertisements

Ideal Operational Amplifier analysis and design
Operational Amplifier
Summing Amplifier -+-+ RFRF R4R4 + IFIF I4I4 VoVo R3R3 + I3I3 V3V3 V4V4 R2R2 + I2I2 V2V2 R1R1 + I1I1 V1V1 RLRL V id.
ECE201 Lect-161 Operational Amplifiers ( ) Dr. Holbert April 3, 2006.
Chapter 18 Operational Amplifiers. The typical op amp has a differential input and a single-ended output. Class B push-pull emitter follower Diff amp.
ECEN 301Discussion #18 – Operational Amplifiers1 Give to Receive Alma 34:28 28 And now behold, my beloved brethren, I say unto you, do not suppose that.
Principles & Applications Operational Amplifiers
CHAPTER 1: INTRODUCTION TO OPERATIONAL AMPLIFIERS
Operational Amplifiers
EECS 40 Spring 2003 Lecture 9S. Ross and W. G. OldhamCopyright Regents of the University of California DIFFERENTIAL AMPLIFIER +  A V+V+ VV V0V0 Differential.
8C Inleiding Meten en Modellen – 8C120 Prof.dr.ir. Bart ter Haar Romeny Dr. Andrea Fuster Faculteit Biomedische Technologie Biomedische Beeld.
Lecture 91 Loop Analysis (3.2) Circuits with Op-Amps (3.3) Prof. Phillips February 19, 2003.
Chapter 2 – Operational Amplifiers
Op Amps Lecture 30.
Chapter 2 – Operational Amplifiers Introduction Textbook CD
Lecture 9: Operational Amplifiers
1 ECE 3336 Introduction to Circuits & Electronics MORE on Operational Amplifiers Spring 2015, TUE&TH 5:30-7:00 pm Dr. Wanda Wosik Set #14.
Operational Amplifiers
Content Op-amp Application Introduction Inverting Amplifier
Operational Amplifiers
IDEAL OPERATIONAL AMPLIFIER AND OP-AMP CIRCUITS
“Op-Amp” Operational Amplifier Non Inverting Amplifier Inverting Amplifier Adder –(and Subtractor using an Inverter) Differential Amplifier Integrator.
ECE 340 ELECTRONICS I OPERATIONAL AMPLIFIERS. OPERATIONAL AMPLIFIER THEORY OF OPERATION CHARACTERISTICS CONFIGURATIONS.
Introduction to Op Amp Circuits ELEC 121. April 2004ELEC 121 Op Amps2 Basic Op-Amp The op-amp is a differential amplifier with a very high open loop gain.
Objective of Lecture Apply the ‘almost ideal’ op amp model in the following circuits: Inverting Amplifier Noninverting Amplifier Voltage Follower Summing.
Analog Electronics Lecture 5.
Ideal Op-Amp Input impedance of op-amp is ∞ – No current flow in or out of input terminals Output impedance of op-amp (with respect to ground) is ‘0’ –
Chapter 8 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
09/16/2010© 2010 NTUST Today Course overview and information.
© 2012 Pearson Education. Upper Saddle River, NJ, All rights reserved. Electronic Devices, 9th edition Thomas L. Floyd Electronic Devices Ninth.
© 2013 The McGraw-Hill Companies, Inc. All rights reserved. McGraw-Hill 9-1 Electronics Principles & Applications Eighth Edition Chapter 9 Operational.
Microprocessor Interface
Electronics Principles & Applications Fifth Edition Chapter 9 Operational Amplifiers ©1999 Glencoe/McGraw-Hill Charles A. Schuler.
The signal conditioner -- changes the voltage Amplify Attenuate Filter.
Higher Physics – Unit 2 2.4Analogue Electronics. Op-Amp An op-amp has two inputs and one output. The symbol for an op-amp is: inverting input non-inverting.
What is an Op Amp? Ideal Op Amps Applications Examples Lecture 9. Op Amps I 1.
ECE 342 – Jose Schutt-Aine 1 ECE 342 Solid-State Devices & Circuits 18. Operational Amplifiers Jose E. Schutt-Aine Electrical & Computer Engineering University.
Module 4 Operational Amplifier
1 ANALOG ELECTRONICS II Frequency Compensation  the technique of modifying open-loop gain  the purpose is to ensure that op-amp circuits will be stable.
1 EK307 – Electric Circuit Theory Late Entry Accelerated Program Welcome to LEAP Online...
EE 1270 Introduction to Electric Circuits Suketu Naik 0 EE 1270: Introduction to Electric Circuits Lecture 13: Operational Amplifiers Part 1 Chapter 5.
1 Analogue Electronic 2 EMT 212 Chapter 2 Op-Amp Applications and Frequency Response By En. Tulus Ikhsan Nasution.
1 The Operational Amplifier continued The voltage follower provides unity gain, however, the output impedance is changed according to the o/p impedance.
Fundamentals of Electric Circuits Chapter 5 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
1 Op-Amp Imperfections in The Linear Range of Operations Gain and Bandwidth Limitations  Ideal op amps have infinite open-loop gain magnitude (A oL is.
Basic Electronics Ninth Edition Basic Electronics Ninth Edition ©2002 The McGraw-Hill Companies Grob Schultz.
Chapter 30 Operational Amplifiers. 2 Introduction Characteristics –High input impedance –Low output impedance –High open-loop gain –Two inputs –One output.
1 Module 12 Operational Amplifiers – Part II 2 Review from Operational Amplifiers I: Negative inputPositive inputOutput V POS –V NEG Power Supply Voltages.
CHEM*3440 Operational Amplifiers These integrated circuits form the backbone of modern instrumental methods. Understanding their operation will help you.
EE2301: Basic Electronic Circuit Amplifiers - Unit 1: Amplifier Model1 Block D: Amplifiers.
Operational Amplifiers Op Amps – a useful building block K. El-Ayat 11.
1 Amplifiers. Equivalent Circuit of a Voltage Amplifier G vo V i IoIo RoRo VoVo ViVi RiRi IiIi Amplifier ViVi VoVo (a) Black Box Representation.
Amplifiers. BASIC AMPLIFIER CONCEPTS Ideally, an amplifier produces an output signal with identical waveshape as the input signal, but with a larger.
Applications of OP-AMP. Introduction Operational amplifier using IC's is inexpensive, versatile and easy to use. For this reason they are used not only.
REAL OP-AMP LIMITATIONS
OP-AMP APPLICATIONS CONSTANT-GAIN MULTIPLIER CONTROLLED SOURCES INSTRUMENTATION AMPLIFIER.
CONSTANT-GAIN MULTIPLIER CONTROLLED SOURCES INSTRUMENTATION AMPLIFIER
Op-amp used as a summing amplifier or adder It is possible to apply more than one input signal to an inverting amplifier. This circuit will then add all.
1 Operational Amplifiers n Ideal Op-Amp –input terminals –differential gain, open-loop gain.
OP-AMPs Op Amp is short for operational amplifier. An operational amplifier is modeled as a voltage controlled voltage source. An operational amplifier.
Lecture VIII Operational Amplifiers DMT 231/3 Electronic II.
ECE201 Lect-131 Loop Analysis (7.8) Circuits with Op-Amps (3.3) Dr. Holbert October 9, 2001.
© From J. G. Webster (ed.), Medical instrumentation: application and design. 3 rd ed. New York: John Wiley & Sons, Figure 3.1 Op-amp equivalent circuit.
OPERATIONAL AMPLIFIERS + - Presented by D.Satishkumar Asst. Professor, Electrical & Electronics Engineering
EE101-Lecture 8 Operational Amplifier Basics of amplifiers EE101 Fall 2012 Lect 8- Kang1 Noninverting amplifier & Inverting amplifier.
Ref:080114HKNOperational Amplifier1 Op-Amp Properties (1)Infinite Open Loop gain -The gain without feedback -Equal to differential gain -Zero common-mode.
Module 2 Operational Amplifier Basics
BIOPOTENTIAL AMPLIFIERS
Open book, open notes, bring a calculator
Presentation transcript:

Inverting Amplifier Under stable linear operation – A OL = ∞, R in = ∞ – V o = A OL (V in(+) – V in(-) ) – V id = (V in(+) – V in(-) ) = V o /A OL = 0 V – I 1 = V in /R 1 – I B(+) = I B(-) = 0 – I F = -I 1 – V o = I F R F = -I 1 R F = -V in R F /R 1 – Closed loop voltage gain of circuit A CL = V o /V in = -(R f /R i ) VoVo -+-+ RFRF R1R1 V in + - IFIF I1I1 V id I B(+) I B(-) Virtual ground

Summing Amplifier Circuit yields the weighted sum of different input voltages Each input voltage is connected to the negative input terminal of the op-amp by an individual resistor -+-+ RFRF R4R4 + IFIF I4I4 VoVo R3R3 + I3I3 V3V3 V4V4 R2R2 + I2I2 V2V2 R1R1 + I1I1 V1V1

Summing Amplifier KCL current law: I F = I 1 + I 2 + I 3 + I 4 I 1 = V 1 /R 1, I 2 = V 2 /R 2, I 3 = V 3 /R 3, I 4 = V 4 /R 4 I F = -V 0 /R F -V 0 /R F = V 1 /R 1 + V 2 /R 2 + V 3 /R 3 + V 4 /R 4 V 0 = -R F (V 1 /R 1 + V 2 /R 2 + V 3 /R 3 + V 4 /R 4 )

Noninverting Amplifier Under stable linear operation – A OL = ∞, R in = ∞; i in =0 and i 2 =0, – V id = 0; V in = V f – V f = V o β = V o [R 1 /(R 1 +R F )] – V in = V o [R 1 /(R 1 +R F )] – Closed loop voltage gain of circuit A CL = V o /V in = (R 1 +R F )/R 1 VoVo -+-+ RFRF VfVf R1R1 V in V id i2i2 i in

Differential Amplifier Op-amp should amplify V 1 and V 2 equally Above is possible if R 1 = R 2 and R 1F = R 2F V 3 = V 2 {R 2F /(R 2 + R 2F )} I = (V 1 – V 3 )/R 1 = (V 3 – V 0 )/R 1F (V 3 – V 0 ) = (V 1 – V 3 ) R 1F /R 1 V 0 = V 3 (1+ R 1F /R 1 ) - V 1 R 1F /R 1 = V 2 {R 2F /(R 2 + R 2F )} {(R 1 +R 1F )/R 1 } – (V 1 R 1F /R 1 ) =V 2 (R 1F /R 1 ) – (V 1 R 1F /R 1 ) V 0 = (V 2 – V 1 ) (R 1F /R 1 ) VoVo -+-+ R 1F R1R1 I V1V1 V2V2 R2R2 R 2F V3V3 I

Comparators Circuit that compares the input voltage with a reference voltage If (V in + V ref ) > 0 – V 0 = -13 V Else V 0 = +13 V VoVo -+-+ R2R2 R1R1 V in V ref R1R1

Rectifiers Full-wave rectifier circuit using one op-amp If V in < 0, circuit behaves like an inverting amplifier rectifier with gain = 0.5 If V in > 0, the op-amp disconnects and passive resistor chain yields a gain = 0.5 VoVo -+-+ R F = 1K R 1 =2K V in R L = 3K

Effect of Negative Feedback on Output Resistance R oF = R o /(1+βA OL ) For inverting amplifier – β = R 1 /R F For noninverting amplifier – β = R 1 /(R 1 +R F )

Typical Bode Plots elexp.com, people.seas.harvard.edu/

Bandwidth Limitations f c (corner frequency or break frequency or critical frequency): frequency at which the gain of the op-amp deviates from the passband gain f c frequency at which gain of op-amp has dropped 3 dB from passband gain Midband: range of frequencies from 0 to f c Bandwidth: range of frequencies for which gain of op-amp is within 3 dB of maximum Unity gain: 0 dB gain (numerical gain is 1)

Bandwidth Limitations f unity gain = frequency at which A OL = 1 Gain-Bandwidth Product (GBW) = numerical closed loop gain value X frequency For both inverting and noninverting amplifiers – f c = f unity / {1+(R F /R 1 )}

Cascaded Amplifiers Total gain = A CL1 A CL2 Overall bandwidth (BW T ) = BW s √(2 1/n -1) – Where n is the number of stages cascaded R R R V in VoVo A1A1 A2A2