Section J8b: FET Low Frequency Response

Similar documents
Lecture 17: Frequency Response of Amplifiers

UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences

General Considerations Miller Effect Association of Poles with Nodes Common Source Stage Source Follower Differential Pair

Chapter 17 Amplifier Frequency Response

CHAPTER 13 FILTERS AND TUNED AMPLIFIERS

ECEN326: Electronic Circuits Fall 2017

Introduction to CMOS RF Integrated Circuits Design

55:041 Electronic Circuits

Dimensional Analysis A Tool for Guiding Mathematical Calculations

Social Studies 201 Notes for November 14, 2003

TP A.30 The effect of cue tip offset, cue weight, and cue speed on cue ball speed and spin

Scale Efficiency in DEA and DEA-R with Weight Restrictions

Topic 7 Fuzzy expert systems: Fuzzy inference

Conservation of Energy

MAE140 Linear Circuits Fall 2012 Final, December 13th

Question 1 Equivalent Circuits

HY:433 Σχεδίαση Αναλογικών/Μεικτών και Υψισυχνών Κυκλωμάτων

The Operational Amplifier

Lecture 6: Resonance II. Announcements

Control Systems Analysis and Design by the Root-Locus Method

Practice Midterm #1 Solutions. Physics 6A

Introduction to Laplace Transform Techniques in Circuit Analysis

The Extended Balanced Truncation Algorithm

Lecture 10 Filtering: Applied Concepts

Lecture 36: MOSFET Common Drain (Source Follower) Amplifier.

Lecture 12 - Non-isolated DC-DC Buck Converter

Lecture 2 Phys 798S Spring 2016 Steven Anlage. The heart and soul of superconductivity is the Meissner Effect. This feature uniquely distinguishes

DIFFERENTIAL EQUATIONS

Department of Mechanical Engineering Massachusetts Institute of Technology Modeling, Dynamics and Control III Spring 2002

Chapter 4. The Laplace Transform Method

Lecture 4 Topic 3: General linear models (GLMs), the fundamentals of the analysis of variance (ANOVA), and completely randomized designs (CRDs)

Design By Emulation (Indirect Method)

Gain and Phase Margins Based Delay Dependent Stability Analysis of Two- Area LFC System with Communication Delays

FUNDAMENTALS OF POWER SYSTEMS

If Y is normally Distributed, then and 2 Y Y 10. σ σ

SERIES COMPENSATION: VOLTAGE COMPENSATION USING DVR (Lectures 41-48)

7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281

On the Use of High-Order Moment Matching to Approximate the Generalized-K Distribution by a Gamma Distribution

Chapter 7. Principles of Unsteady - State and Convective Mass Transfer

Linearteam tech paper. The analysis of fourth-order state variable filter and it s application to Linkwitz- Riley filters

SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuits II. Solutions to Assignment 3 February 2005.

Image Denoising Based on Non-Local Low-Rank Dictionary Learning

4 Conservation of Momentum

EE 508 Lecture 16. Filter Transformations. Lowpass to Bandpass Lowpass to Highpass Lowpass to Band-reject

Several schematic symbols for a capacitor are shown below. The symbol resembles the two conducting surfaces separated with a dielectric.

AP Physics Momentum AP Wrapup

Suggestions - Problem Set (a) Show the discriminant condition (1) takes the form. ln ln, # # R R

Lecture 4. Chapter 11 Nise. Controller Design via Frequency Response. G. Hovland 2004

EE 508 Lecture 16. Filter Transformations. Lowpass to Bandpass Lowpass to Highpass Lowpass to Band-reject

SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuits II. R 4 := 100 kohm

Chapter 10 Transistor amplifier design

Lecture 10 OUTLINE. Reading: Chapter EE105 Spring 2008 Lecture 10, Slide 1 Prof. Wu, UC Berkeley

Fig.L3.1. A cross section of a MESFET (a) and photograph and electrode layout (b).

Lecture #9 Continuous time filter

into a discrete time function. Recall that the table of Laplace/z-transforms is constructed by (i) selecting to get

Chapter 5 Consistency, Zero Stability, and the Dahlquist Equivalence Theorem

Tuning of High-Power Antenna Resonances by Appropriately Reactive Sources

Highway Capacity Manual 2010

online learning Unit Workbook 4 RLC Transients

PHYSICS 151 Notes for Online Lecture 2.3

11.2 Stability. A gain element is an active device. One potential problem with every active circuit is its stability

Section Induction motor drives

Frequency Response of Amplifiers

Social Studies 201 Notes for March 18, 2005

The Electric Potential Energy

UNIT 15 RELIABILITY EVALUATION OF k-out-of-n AND STANDBY SYSTEMS

ECE 3510 Root Locus Design Examples. PI To eliminate steady-state error (for constant inputs) & perfect rejection of constant disturbances

ADAPTIVE CONTROL DESIGN FOR A SYNCHRONOUS GENERATOR

s s 1 s = m s 2 = 0; Δt = 1.75s; a =? mi hr

NOTE: The items d) and e) of Question 4 gave you bonus marks.

EE 4443/5329. LAB 3: Control of Industrial Systems. Simulation and Hardware Control (PID Design) The Inverted Pendulum. (ECP Systems-Model: 505)

Per Unit Analysis. Single-Phase systems

Physics 20 Lesson 16 Friction

Kalman Filter. Wim van Drongelen, Introduction

Clustering Methods without Given Number of Clusters

EECS240 Spring Lecture 13: Settling. Lingkai Kong Dept. of EECS

Part A: Signal Processing. Professor E. Ambikairajah UNSW, Australia

Module 4: Time Response of discrete time systems Lecture Note 1

Chapter 2 Sampling and Quantization. In order to investigate sampling and quantization, the difference between analog

Name: Answer Key Date: Regents Physics. Energy

Zbigniew Dziong Department of Electrical Engineering, Ecole de Technologie Superieure 1100 Notre-Dame Street West, Montreal, Quebec, Canada H3C 1k3

CHAPTER 5. The Operational Amplifier 1

Nonlinear Single-Particle Dynamics in High Energy Accelerators

12.4 Atomic Absorption and Emission Spectra

Given the following circuit with unknown initial capacitor voltage v(0): X(s) Immediately, we know that the transfer function H(s) is

Preemptive scheduling on a small number of hierarchical machines

μ + = σ = D 4 σ = D 3 σ = σ = All units in parts (a) and (b) are in V. (1) x chart: Center = μ = 0.75 UCL =

THE BICYCLE RACE ALBERT SCHUELLER

Improving the Efficiency of a Digital Filtering Scheme for Diabatic Initialization

HOMEWORK ASSIGNMENT #2

CHAPTER 14 SIGNAL GENERATORS AND WAVEFORM-SHAPING CIRCUITS

Source slideplayer.com/fundamentals of Analytical Chemistry, F.J. Holler, S.R.Crouch. Chapter 6: Random Errors in Chemical Analysis

5.5 Application of Frequency Response: Signal Filters

Linear Motion, Speed & Velocity

A Full-Newton Step Primal-Dual Interior Point Algorithm for Linear Complementarity Problems *

What lies between Δx E, which represents the steam valve, and ΔP M, which is the mechanical power into the synchronous machine?

Chapter 2 Homework Solution P2.2-1, 2, 5 P2.4-1, 3, 5, 6, 7 P2.5-1, 3, 5 P2.6-2, 5 P2.7-1, 4 P2.8-1 P2.9-1

Publication V by authors

CISE302: Linear Control Systems

Chapter 7. Root Locus Analysis

Transcription:

ection J8b: FET ow Frequency epone In thi ection of our tudie, we re o to reiit the baic FET aplifier confiuration but with an additional twit The baic confiuration are the ae a we etiated ection J6 of the WebT note, with the iilaritie and difference a noted the table below: Then External capacitor bypa & coupl Ideal hort for ac Tranitor output Very lare reitance, r o ay uually be ored Input and output eitance characteritic, out FET pproxiation i, o i i Now Non-ideal keep all al circuit OK, we ll keep thi one Ipedance Z, Z out OK, unle otherwie noted Jut like we did for the BJT confiuration, we re o to tart by look at each of the baic aplifier tae ter of analyi and fih with trateie for de for a pecific low frequency characteritic ll aplifier are preented a capacitie-coupled to tae that ay occur before and after ecall that thi i the eaiet way to enure dc iolation, but ay not be feaible certa circutance or under certa condition Note: the circuit that follow, the actual al ource and it aociated ource reitance ource hae been cluded reiouly, we knew that thi ource and reitance wa there but we jut tarted our etiation with the put to the tranitor Thi hould not caue too uch heartburn the analyi proce i the ae and the relationhip between and i a oltae diider ce we e already ot an FET circuit the ource le, don t et confued between the ource of the tranitor itelf and the reitance aociated with the al ource hown a orry, I know it confu! ow Frequency epone of the oon-ource plifier To facilitate the analyi of the FET aplifier confiuration, the ot coplicated confiuration i addreed firt Thi will allow u to detere all tie contant and the analyi of the ipler confiuration will ole the eliation of appropriate ter lo recall that JFET and MOFET circuit are analyzed the ae way thi alo hold here that the tie contant do not depend on the type of FET

The JFET ipleentation of the coon-ource aplifier i ien to the left below, and the odified all al odel i to the riht below baed on Fiure 9a and 9b of your text ett the put ource,, equal to zero reult the circuit ien to the riht that we will ue for analyi purpoe U thi circuit, and the oberation that the dependent current ource i opened ce, we can fd the equialent reitance een by,, and our old friend, the Method of hort ircuit Tie ontant : ett and equal to fity hort circuit, the equialent reitance een by i, where for the confiuration : ett the ipedance of and be equal to zero, the equialent reitance een by i

: ett the ipedance of and be equal to zero, the equialent reitance een by i Note that, jut a for the cae of the coon-eitter aplifier, the bypa capacitor troduce a zero at Z Z The coupl acitor each troduce a z cap ero at zero frequency The tie contant for the aplifier are therefore defed by ; ;, and the lower corner frequency i crudely approxiated by, ith a better approxiation ien by -ource aplifier, where only part of the ource reitance i bypaed, i ien by w Z Z The idband oltae a for the coon idband, and the noralized frequency dependent a expreion i ien by Z idband

ow Frequency epone of the ource-follower plifier The eneric circuit for the FET F aplifier u an n-channel JFET i illutrated the fiure to the left below The odified all al equialent circuit i hown below and to the riht baed on Fiure a and b of your text The ource-follower, or coondra, FET aplifier i iilar to the EF aplifier, it BJT counterpart It alo ha two tie contant, one of which i uch larer than the other The circuit ued to derie the tie contant of the circuit capacitor i ien to the riht : The equialent reitance een by the coupl capacitor i found by ett equal to fity, or, where the put reitance for an F aplifier wa preiouly defed a : The equialent reitance een by the coupl capacitor i equal to

Note that thi equialent reitance i not directly oberable fro the aboe fiure Intead, the Theen oltae and current are defed, with the equialent reitance be equal to the Theen reitance e for a ien Frequency haracteritic e an FET aplifier for a pecified low frequency repone i a outled ection H3 for BJT aplifier and i reproduced follow: pproach : If the pole can be eparated by at leat a decade, we let one doant pole produce the entire 3dB drop Thi i iilar to the cae of a le pole, ce there i irtually no teraction between the two the frequency oe to zero, the doant pole at the hiher frequency will defe the corner frequency before the econd pole be to take effect pproach : If the put and output reitance are approxiately equal, we et the two pole frequencie to be equal; ie, we hae a double pole Thi ean that each pole contribute eenly at the break pot or, equialently, that each pole contribute a 5dB drop o that the total decreae will be 3dB at the deired corner frequency For exaple, a noralized oltae a expreion with each pole at frequency, i ien by idband If we further pecify that we want thi noralized a to hae a anitude of 77-3dB at a corner frequency, j idband j j ol for the frequency of the double pole ter of the pecified corner frequency, we et Equation 4 55 Note that the actual frequency of the double pole i below the pecified de corner frequency Thi i to be expected, ce the pole are

teract if each had been located at, there would hae been a 6dB drop tead of the 3dB deired pproach 3: The firt two approache achieed the deired corner frequency by controll pole placeent In contrat, thi ethod chooe equal capacitor alue, a technique that will allow for terchan of coponent a retrict ourele to a two-pole yte with pole frequencie and, we et the expreion for the noralized a anitude equal to 77 at the pecified corner frequency, : idband j j j ol the aboe expreion for, we et 4 If and are both le than, the lat ter the aboe expreion ay be nelected and we can ole for a Equation 7, Modified Once we et to thi pot, it depend on the actual copoition of the tie contant aociated with and The tratey i to et the capacitor of each pole equal Know the reitie coponent the equialent reitance and the deired corner frequency, the capacitor alue i the only unknown Equation 7 the odified erion aboe and ay be calculated