AD8476 Fully Differential Unity Gain Amplifier and ADC Driver (Rev. B)
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ECE 255, MOSFET Basic Configurations
ECE 255, MOSFET Basic Configurations 8 March 2018 In this lecture, we will go back to Section 7.3, and the basic configurations of MOSFET amplifiers will be studied similar to that of BJT. Previously, it has been shown that with the transistor DC biased at the appropriate point (Q point or operating point), linear relations can be derived between the small voltage signal and current signal. We will continue this analysis with MOSFETs, starting with the common-source amplifier. 1 Common-Source (CS) Amplifier The common-source (CS) amplifier for MOSFET is the analogue of the common- emitter amplifier for BJT. Its popularity arises from its high gain, and that by cascading a number of them, larger amplification of the signal can be achieved. 1.1 Chararacteristic Parameters of the CS Amplifier Figure 1(a) shows the small-signal model for the common-source amplifier. Here, RD is considered part of the amplifier and is the resistance that one measures between the drain and the ground. The small-signal model can be replaced by its hybrid-π model as shown in Figure 1(b). Then the current induced in the output port is i = −gmvgs as indicated by the current source. Thus vo = −gmvgsRD (1.1) By inspection, one sees that Rin = 1; vi = vsig; vgs = vi (1.2) Thus the open-circuit voltage gain is vo Avo = = −gmRD (1.3) vi Printed on March 14, 2018 at 10 : 48: W.C. Chew and S.K. Gupta. 1 One can replace a linear circuit driven by a source by its Th´evenin equivalence. -
Chapter 10 Differential Amplifiers
Chapter 10 Differential Amplifiers 10.1 General Considerations 10.2 Bipolar Differential Pair 10.3 MOS Differential Pair 10.4 Cascode Differential Amplifiers 10.5 Common-Mode Rejection 10.6 Differential Pair with Active Load 1 Audio Amplifier Example An audio amplifier is constructed as above that takes a rectified AC voltage as its supply and amplifies an audio signal from a microphone. CH 10 Differential Amplifiers 2 “Humming” Noise in Audio Amplifier Example However, VCC contains a ripple from rectification that leaks to the output and is perceived as a “humming” noise by the user. CH 10 Differential Amplifiers 3 Supply Ripple Rejection vX Avvin vr vY vr vX vY Avvin Since both node X and Y contain the same ripple, their difference will be free of ripple. CH 10 Differential Amplifiers 4 Ripple-Free Differential Output Since the signal is taken as a difference between two nodes, an amplifier that senses differential signals is needed. CH 10 Differential Amplifiers 5 Common Inputs to Differential Amplifier vX Avvin vr vY Avvin vr vX vY 0 Signals cannot be applied in phase to the inputs of a differential amplifier, since the outputs will also be in phase, producing zero differential output. CH 10 Differential Amplifiers 6 Differential Inputs to Differential Amplifier vX Avvin vr vY Avvin vr vX vY 2Avvin When the inputs are applied differentially, the outputs are 180° out of phase; enhancing each other when sensed differentially. CH 10 Differential Amplifiers 7 Differential Signals A pair of differential signals can be generated, among other ways, by a transformer. -
Differential Amplifiers
www.getmyuni.com Operational Amplifiers: The operational amplifier is a direct-coupled high gain amplifier usable from 0 to over 1MH Z to which feedback is added to control its overall response characteristic i.e. gain and bandwidth. The op-amp exhibits the gain down to zero frequency. Such direct coupled (dc) amplifiers do not use blocking (coupling and by pass) capacitors since these would reduce the amplification to zero at zero frequency. Large by pass capacitors may be used but it is not possible to fabricate large capacitors on a IC chip. The capacitors fabricated are usually less than 20 pf. Transistor, diodes and resistors are also fabricated on the same chip. Differential Amplifiers: Differential amplifier is a basic building block of an op-amp. The function of a differential amplifier is to amplify the difference between two input signals. How the differential amplifier is developed? Let us consider two emitter-biased circuits as shown in fig. 1. Fig. 1 The two transistors Q1 and Q2 have identical characteristics. The resistances of the circuits are equal, i.e. RE1 = R E2, RC1 = R C2 and the magnitude of +VCC is equal to the magnitude of �VEE. These voltages are measured with respect to ground. To make a differential amplifier, the two circuits are connected as shown in fig. 1. The two +VCC and �VEE supply terminals are made common because they are same. The two emitters are also connected and the parallel combination of RE1 and RE2 is replaced by a resistance RE. The two input signals v1 & v2 are applied at the base of Q1 and at the base of Q2. -
INA106: Precision Gain = 10 Differential Amplifier Datasheet
INA106 IN A1 06 IN A106 SBOS152A – AUGUST 1987 – REVISED OCTOBER 2003 Precision Gain = 10 DIFFERENTIAL AMPLIFIER FEATURES APPLICATIONS ● ACCURATE GAIN: ±0.025% max ● G = 10 DIFFERENTIAL AMPLIFIER ● HIGH COMMON-MODE REJECTION: 86dB min ● G = +10 AMPLIFIER ● NONLINEARITY: 0.001% max ● G = –10 AMPLIFIER ● EASY TO USE ● G = +11 AMPLIFIER ● PLASTIC 8-PIN DIP, SO-8 SOIC ● INSTRUMENTATION AMPLIFIER PACKAGES DESCRIPTION R1 R2 10kΩ 100kΩ 2 5 The INA106 is a monolithic Gain = 10 differential amplifier –In Sense consisting of a precision op amp and on-chip metal film 7 resistors. The resistors are laser trimmed for accurate gain V+ and high common-mode rejection. Excellent TCR tracking 6 of the resistors maintains gain accuracy and common-mode Output rejection over temperature. 4 V– The differential amplifier is the foundation of many com- R3 R4 10kΩ 100kΩ monly used circuits. The INA106 provides this precision 3 1 circuit function without using an expensive resistor network. +In Reference The INA106 is available in 8-pin plastic DIP and SO-8 surface-mount packages. Please be aware that an important notice concerning availability, standard warranty, and use in critical applications of Texas Instruments semiconductor products and disclaimers thereto appears at the end of this data sheet. All trademarks are the property of their respective owners. PRODUCTION DATA information is current as of publication date. Copyright © 1987-2003, Texas Instruments Incorporated Products conform to specifications per the terms of Texas Instruments standard warranty. Production processing does not necessarily include testing of all parameters. www.ti.com SPECIFICATIONS ELECTRICAL ° ± At +25 C, VS = 15V, unless otherwise specified. -
Transistor Basics
Transistor Basics: Collector The schematic representation of a transistor is shown to the left. Note the arrow pointing down towards the emitter. This signifies it's an NPN transistor (current flows in the direction of the arrow). See the Q1 datasheet at: www.fairchildsemi.com. Base 2N3904 A transistor is basically a current amplifier. Say we let 1mA flow into the base. We may get 100mA flowing into the collector. Note: The Emitter currents flowing into the base and collector exit through the emitter (the sum off all currents entering or leaving a node must equal zero). The gain of the transistor will be listed in the datasheet as either βDC or Hfe. The gain won't be identical even in transistors with the same part number. The gain also varies with the collector current and temperature. Because of this we will add a safety margin to all our base current calculations (i.e. if we think we need 2mA to turn on the switch we'll use 4mA just to make sure). Sample circuit and calculations (NPN transistor): Let's say we want to heat a block of metal. One way to do that is to connect a power resistor to the block and run current through the resistor. The resistor heats up and transfers some of the heat to the block of metal. We will use a transistor as a switch to control when the resistor is heating up and when it's cooling off (i.e. no current flowing in the resistor). In the circuit below R1 is the power resistor that is connected to the object to be heated. -
621 212 Electronics and Communication Engineering Ec6304/Linear Integrated Circuits
DSEC/ECE/EC6304-LIC/QB 1 DHANALAKSHMI SRINIVASAN ENGINEERING COLLEGE -621 212 ELECTRONICS AND COMMUNICATION ENGINEERING EC6304/LINEAR INTEGRATED CIRCUITS QUESTION BANK UNIT 1(2 MARKS) 1. What is an integrated circuit? APRIL/MAY 2010 An integrated circuit (IC) is a miniature, low cost electronic circuit consisting of active and Passive components fabricated together on a single crystal of silicon. The active components are Transistors and diodes and passive components are resistors and capacitors. 2. What is current mirror? APRIL/MAY 2010 A constant current source (current mirror) makes use of the fact that for a transistor in the active mode of operation, the collector current is relatively independent of the collector voltage 3. What are two requirements to be met for a good current source? MAY/JUNE 2012 a. Superior insensitivity of circuit performance to power supply variations and temperature. b. More economical than resistors in terms of die area required providing bias currents of small value. c. When used as load element, the high incremental resistance of current source results in high voltage gains at low supply voltages. 4. What are all the important characteristics of ideal op-amp? APRIL/MAY 2015 Ideal characteristics of OPAMP 1. Open loop gain infinite 2. Input impedance infinite 3. Output impedance low 4. Bandwidth infinite 5. Zero offset, ie, Vo=0 when V1=V2=0 5. Define CMRR of OP-AMP APRIL/MAY 2011 The relative sensitivity of an op-amp to a difference signal as compared to a common - mode signal is called the common -mode rejection ratio. It is expressed in decibels. -
S-Parameter Techniques – HP Application Note 95-1
H Test & Measurement Application Note 95-1 S-Parameter Techniques Contents 1. Foreword and Introduction 2. Two-Port Network Theory 3. Using S-Parameters 4. Network Calculations with Scattering Parameters 5. Amplifier Design using Scattering Parameters 6. Measurement of S-Parameters 7. Narrow-Band Amplifier Design 8. Broadband Amplifier Design 9. Stability Considerations and the Design of Reflection Amplifiers and Oscillators Appendix A. Additional Reading on S-Parameters Appendix B. Scattering Parameter Relationships Appendix C. The Software Revolution Relevant Products, Education and Information Contacting Hewlett-Packard © Copyright Hewlett-Packard Company, 1997. 3000 Hanover Street, Palo Alto California, USA. H Test & Measurement Application Note 95-1 S-Parameter Techniques Foreword HEWLETT-PACKARD JOURNAL This application note is based on an article written for the February 1967 issue of the Hewlett-Packard Journal, yet its content remains important today. S-parameters are an Cover: A NEW MICROWAVE INSTRUMENT SWEEP essential part of high-frequency design, though much else MEASURES GAIN, PHASE IMPEDANCE WITH SCOPE OR METER READOUT; page 2 See Also:THE MICROWAVE ANALYZER IN THE has changed during the past 30 years. During that time, FUTURE; page 11 S-PARAMETERS THEORY AND HP has continuously forged ahead to help create today's APPLICATIONS; page 13 leading test and measurement environment. We continuously apply our capabilities in measurement, communication, and computation to produce innovations that help you to improve your business results. In wireless communications, for example, we estimate that 85 percent of the world’s GSM (Groupe Speciale Mobile) telephones are tested with HP instruments. Our accomplishments 30 years hence may exceed our boldest conjectures. -
Fully-Differential Amplifiers
Application Report S Fully-Differential Amplifiers James Karki AAP Precision Analog ABSTRACT Differential signaling has been commonly used in audio, data transmission, and telephone systems for many years because of its inherent resistance to external noise sources. Today, differential signaling is becoming popular in high-speed data acquisition, where the ADC’s inputs are differential and a differential amplifier is needed to properly drive them. Two other advantages of differential signaling are reduced even-order harmonics and increased dynamic range. This report focuses on integrated, fully-differential amplifiers, their inherent advantages, and their proper use. It is presented in three parts: 1) Fully-differential amplifier architecture and the similarities and differences from standard operational amplifiers, their voltage definitions, and basic signal conditioning circuits; 2) Circuit analysis (including noise analysis), provides a deeper understanding of circuit operation, enabling the designer to go beyond the basics; 3) Various application circuits for interfacing to differential ADC inputs, antialias filtering, and driving transmission lines. Contents 1 Introduction . 3 2 What Is an Integrated, Fully-Differential Amplifier? . 3 3 Voltage Definitions . 5 4 Increased Noise Immunity . 5 5 Increased Output Voltage Swing . 6 6 Reduced Even-Order Harmonic Distortion . 6 7 Basic Circuits . 6 8 Circuit Analysis and Block Diagram . 8 9 Noise Analysis . 13 10 Application Circuits . 15 11 Terminating the Input Source . 15 12 Active Antialias Filtering . 20 13 VOCM and ADC Reference and Input Common-Mode Voltages . 23 14 Power Supply Bypass . 25 15 Layout Considerations . 25 16 Using Positive Feedback to Provide Active Termination . 25 17 Conclusion . 27 1 SLOA054E List of Figures 1 Integrated Fully-Differential Amplifier vs Standard Operational Amplifier. -
MOS Amplifier Basics
ECE 2C Laboratory Manual 2 MOS Amplifier Basics Overview This lab will explore the design and operation of basic single-transistor MOS amplifiers at mid-band. We will explore the common-source and common-gate configurations, as well as a CS amplifier with an active load and biasing. Table of Contents Pre-lab Preparation 2 Before Coming to the Lab 2 Parts List 2 Background Information 3 Small-Signal Amplifier Design and Biasing 3 MOSFET Design Parameters and Subthreshold Currents 5 Estimating Key Device Parameters 7 In-Lab Procedure 8 2.1 Common-Source Amplifier 8 Common-Source, no Source Resistor 8 Linearity and Waveform Distortion 8 Effect of Source and Load Impedances 9 Common-Source with Source Resistor 9 2.2 Common-Gate Amplifier 10 2.3 Amplifiers with Active Loading 11 Feedback-Bias Amplifier 11 CMOS Active-Load CS Amplifier 12 1 © Bob York 2 MOS Amplifier Basics Pre-lab Preparation Before Coming to the Lab Read through the lab experiment to familiarize yourself with the components and assembly sequence. Before coming to the lab, each group should obtain a parts kit from the ECE Shop. Parts List The ECE2 lab is stocked with resistors so do not be alarmed if you kits does not include the resistors listed below. Some of these parts may also have been provided in an earlier kit. Laboratory #2 MOS Amplifiers Qty Description 2 CD4007 CMOS pair/inverter 4 2N7000 NMOS 4 1uF capacitor (electrolytic, 25V, radial) 8 10uF capacitor (electrolytic, 25V, radial) 4 100uF capacitor (electrolytic, 25V, radial) 4 100-Ohm 1/4 Watt resistor 4 220-Ohm 1/4 Watt resistor 1 470-Ohm 1/4 Watt resistor 4 10-KOhm 1/4 Watt resistor 1 33-KOhm 1/4 Watt resistor 2 47-KOhm 1/4 Watt resistor 1 68-KOhm 1/4 Watt resistor 4 100-KOhm 1/4 Watt resistor 1 1-MOhm 1/4 Watt resistor 1 10k trimpot 2 100k trimpot © Bob York Background Information 3 Background Information Small-Signal Amplifier Design and Biasing In earlier experiments with transistors we learned how to establish a desired DC operating condition. -
Mosfet Differential Amplifier (Two-Week Lab)
page 1 of 7 MOSFET DIFFERENTIAL AMPLIFIER (TWO-WEEK LAB) BACKGROUND The MOSFET is by far the most widely used transistor in both digital and analog circuits, and it is the backbone of modern electronics. One of the most common uses of the MOSFET in analog circuits is the construction of differential amplifiers. The latter are used as input stages in op-amps, video amplifiers, high-speed comparators, and many other analog-based circuits. MOSFET differential amplifiers are used in integrated circuits, such as operational amplifiers, they provide a high input impedance for the input terminals. A properly designed differential amplifier with its current-mirror biasing stages is made from matched-pair devices to minimize imbalances from one side of the differential amplifier to the other. In this lab, you will design a differential amplifier by first verifying its operation in PSPICE, then building and testing your circuit stage by stage. In your lab kit, you will find one or more CD4007 integrated circuits. (The letter prefix may vary; it's the number 4007 that matters.) This IC contains a number of NMOS and PMOS devices, as shown below. You may assume that all the NMOS transistors are matched to each other (same value of K and threshold voltage VTR), and that all the PMOS devices are similarly matched to each other. Use the devices in this integrated circuit when building your differential amplifier, as requested in Levels 2 and 3. page 2 of 7 BACKGROUND The general topology of a differential amplifier is shown below. Two active devices are connected to a positive voltage supply via passive series elements. -
Lsk389 Application Note Dual Monolithic Jfet for Ultra-Low Noise Applications
Over 30 Years of Quality Through Innovation LSK389 APPLICATION NOTE DUAL MONOLITHIC JFET FOR ULTRA-LOW NOISE APPLICATIONS By: Bob Cordell 01/21/2020 REV. A3 Linear Integrated Systems • 4042 Clipper Court • Fremont, CA 94538 • Tel: 510 490-9160 • Fax: 510 353-0261 • Email: [email protected] LINEAR SYSTEMS LSK389 DUAL MONOLITHIC JFET FOR ULTRA-LOW NOISE APPLICATIONS Features Applications ▪ Low Wideband Noise ▪ Low Noise Amplifiers ▪ Low 1/f Noise ▪ Differential Amplifiers ▪ High Transconductance ▪ High Input Impedance Amplifiers ▪ Well-Matched Threshold Voltages ▪ Phono and Other Audio Preamps ▪ High gm/Capacitance Ratio ▪ Condenser Microphone Preamps ▪ Industry's First 100% Noise-Tested JFET ▪ Electrometers ▪ Piezoelectric Sensor Preamps ▪ Front-end for Low-Noise Op Amps Introduction The LSK389 is the industry’s lowest noise Dual N-Channel JFET, 100% tested, guaranteed to meet 1/f and broadband noise specifications, while eliminating burst (RTN or popcorn) noise entirely. The product displays high transconductance and very good matching. It is the JFET of choice for low noise applications, especially those requiring a differential amplifier input stage. LSK389 Key Specifications ▪ 1.3 nV/√Hz input noise at 1 kHz, ID = 2 mA ▪ 1.5 nV/√Hz at 10 Hz, ID = 2 mA ▪ 14 mS transconductance at ID = 2 mA ▪ Improved DC offset ±15 mV max. ▪ CISS = 25 pF typ. ▪ CRSS = 5.5 pF typ. ▪ Breakdown voltage = 40 V min. ▪ 4 grades of IDSS available (A, B, C, D) N-Channel JFET Basics The simplified equation below describes the DC operation of a JFET [1]. The term Vt is the threshold voltage. The term is the transconductance coefficient of the JFET (not to be confused with BJT current gain). -
Fully Differential Op Amps Made Easy
Application Report SLOA099 - May 2002 Fully Differential Op Amps Made Easy Bruce Carter High Performance Linear ABSTRACT Fully differential op amps may be unfamiliar to some designers. This application report gives designers the essential information to get a fully differential design up and running. Contents 1 Introduction . 2 2 What Does Fully Differential Mean?. 2 3 How Is the Second Output Used?. 3 3.1 Differential Gain Stages. 3 3.2 Single-Ended to Differential Conversion. 4 3.3 Working With Terminated Inputs. 5 4 A New Function . 7 5 Conclusions . 8 6 References . 9 List of Figures 1 Single-Ended Op Amp Schematic Symbol. 2 2 Fully Differential Op Amp Schematic Symbol. 2 3 Closing the Loop on a Single-Ended Op Amp. 3 4 Closing the Loop on a Fully Differential Op Amp. 3 5 Single Ended to Differential Conversion. 4 6 Relationship Between Vin, Vout+, and Vout– . 5 7 Fully Differential Amplifier Component Calculator. 6 8 Using a Fully Differential Op Amp to Drive an ADC. 7 9 Effect of Vocm on Vout+ and Vout– . 8 1 SLOA099 1 Introduction Fully differential op amps may be intimidating to some designers, But op amps began as fully differential components over 50 years ago. Techniques about how to use the fully differential versions have been almost lost over the decades. However, today’s fully differential op amps offer performance advantages unheard of in those first units. This report does not attempt a detailed analysis of op amp theory; reference 1 covers theory well. Instead, this report presents just the facts a designer needs to get started, and some resources for further design assistance.