Section J8b: FET Low Frequency Response

Size: px
Start display at page:

Download "Section J8b: FET Low Frequency Response"

Transcription

1 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

2 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

3 : 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

4 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

5 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

6 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

Lecture 17: Frequency Response of Amplifiers

Lecture 17: Frequency Response of Amplifiers ecture 7: Frequency epone of Aplifier Gu-Yeon Wei Diiion of Engineering and Applied Science Harard Unierity guyeon@eec.harard.edu Wei Oeriew eading S&S: Chapter 7 Ski ection ince otly decribed uing BJT

More information

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

UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences UNIVEITY OF CAIFONIA Collee of Enineerin Departent of Electrical Enineerin and Coputer cience E. Alon Hoework # olution EEC 40 P. Nuzzo Ue the EEC40 90n CMO proce in all hoework and project unle noted

More information

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

General Considerations Miller Effect Association of Poles with Nodes Common Source Stage Source Follower Differential Pair Frequency epone of Aplifier General onideration Miller Effect Aociation of Pole with Node oon ource tage ource Follower ifferential Pair Haan Abouhady Univerity of Pari I eference B. azavi, eign of Analog

More information

Chapter 17 Amplifier Frequency Response

Chapter 17 Amplifier Frequency Response hapter 7 Amplifier Frequency epone Microelectronic ircuit Deign ichard. Jaeger Travi N. Blalock 8/0/0 hap 7- hapter Goal eview tranfer function analyi and dominant-pole approximation of amplifier tranfer

More information

CHAPTER 13 FILTERS AND TUNED AMPLIFIERS

CHAPTER 13 FILTERS AND TUNED AMPLIFIERS HAPTE FILTES AND TUNED AMPLIFIES hapter Outline. Filter Traniion, Type and Specification. The Filter Tranfer Function. Butterworth and hebyhev Filter. Firt Order and Second Order Filter Function.5 The

More information

ECEN326: Electronic Circuits Fall 2017

ECEN326: Electronic Circuits Fall 2017 EEN36: Electronic ircuits Fall 07 ecture 5: Frequency esponse a Palero Analo & Mixed-al enter Texas A&M University Announceents HW5 due / Exa /6 9:0-0:0 (0 extra utes) losed book w/ one standard note sheet

More information

Introduction to CMOS RF Integrated Circuits Design

Introduction to CMOS RF Integrated Circuits Design Introduction to CMO F Interated Circuit Dein III. Low Noie Aplifier Introduction to CMO F Interated Circuit Dein Fall 0, Prof. JianJun Zhou III- Outline Fiure of erit Baic tructure Input and output atchin

More information

55:041 Electronic Circuits

55:041 Electronic Circuits 55:04 Electronic ircuit Frequency epone hapter 7 A. Kruger Frequency epone- ee page 4-5 of the Prologue in the text Important eview co Thi lead to the concept of phaor we encountered in ircuit In Linear

More information

Dimensional Analysis A Tool for Guiding Mathematical Calculations

Dimensional Analysis A Tool for Guiding Mathematical Calculations Dimenional Analyi A Tool for Guiding Mathematical Calculation Dougla A. Kerr Iue 1 February 6, 2010 ABSTRACT AND INTRODUCTION In converting quantitie from one unit to another, we may know the applicable

More information

Social Studies 201 Notes for November 14, 2003

Social Studies 201 Notes for November 14, 2003 1 Social Studie 201 Note for November 14, 2003 Etimation of a mean, mall ample ize Section 8.4, p. 501. When a reearcher ha only a mall ample ize available, the central limit theorem doe not apply to the

More information

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

TP A.30 The effect of cue tip offset, cue weight, and cue speed on cue ball speed and spin technical proof TP A.30 The effect of cue tip offet, cue weight, and cue peed on cue all peed and pin technical proof upporting: The Illutrated Principle of Pool and Billiard http://illiard.colotate.edu

More information

Scale Efficiency in DEA and DEA-R with Weight Restrictions

Scale Efficiency in DEA and DEA-R with Weight Restrictions Available online at http://ijdea.rbiau.ac.ir Int. J. Data Envelopent Analyi (ISSN 2345-458X) Vol.2, No.2, Year 2014 Article ID IJDEA-00226, 5 page Reearch Article International Journal of Data Envelopent

More information

Topic 7 Fuzzy expert systems: Fuzzy inference

Topic 7 Fuzzy expert systems: Fuzzy inference Topic 7 Fuzzy expert yte: Fuzzy inference adani fuzzy inference ugeno fuzzy inference Cae tudy uary Fuzzy inference The ot coonly ued fuzzy inference technique i the o-called adani ethod. In 975, Profeor

More information

Conservation of Energy

Conservation of Energy Add Iportant Conervation of Energy Page: 340 Note/Cue Here NGSS Standard: HS-PS3- Conervation of Energy MA Curriculu Fraework (006):.,.,.3 AP Phyic Learning Objective: 3.E.., 3.E.., 3.E..3, 3.E..4, 4.C..,

More information

MAE140 Linear Circuits Fall 2012 Final, December 13th

MAE140 Linear Circuits Fall 2012 Final, December 13th MAE40 Linear Circuit Fall 202 Final, December 3th Intruction. Thi exam i open book. You may ue whatever written material you chooe, including your cla note and textbook. You may ue a hand calculator with

More information

Question 1 Equivalent Circuits

Question 1 Equivalent Circuits MAE 40 inear ircuit Fall 2007 Final Intruction ) Thi exam i open book You may ue whatever written material you chooe, including your cla note and textbook You may ue a hand calculator with no communication

More information

HY:433 Σχεδίαση Αναλογικών/Μεικτών και Υψισυχνών Κυκλωμάτων

HY:433 Σχεδίαση Αναλογικών/Μεικτών και Υψισυχνών Κυκλωμάτων HY:433 Σχεδίαση Αναλογικών/Μεικτών και Υψισυχνών Κυκλωμάτων «Low Noie Aplifier» Φώτης Πλέσσας fplea@e-ce.uth.r F eceiver Antenna BPF LNA BPF Mixer BPF3 IF Ap Deodulator F front end LO LNA De Conideration

More information

The Operational Amplifier

The Operational Amplifier The Operational Amplifier The operational amplifier i a building block of modern electronic intrumentation. Therefore, matery of operational amplifier fundamental i paramount to any practical application

More information

Lecture 6: Resonance II. Announcements

Lecture 6: Resonance II. Announcements EES 5 Spring 4, Lecture 6 Lecture 6: Reonance II EES 5 Spring 4, Lecture 6 Announcement The lab tart thi week You mut how up for lab to tay enrolled in the coure. The firt lab i available on the web ite,

More information

Control Systems Analysis and Design by the Root-Locus Method

Control Systems Analysis and Design by the Root-Locus Method 6 Control Sytem Analyi and Deign by the Root-Locu Method 6 1 INTRODUCTION The baic characteritic of the tranient repone of a cloed-loop ytem i cloely related to the location of the cloed-loop pole. If

More information

Practice Midterm #1 Solutions. Physics 6A

Practice Midterm #1 Solutions. Physics 6A Practice Midter # Solution Phyic 6A . You drie your car at a peed of 4 k/ for hour, then low down to k/ for the next k. How far did you drie, and what wa your aerage peed? We can draw a iple diagra with

More information

Introduction to Laplace Transform Techniques in Circuit Analysis

Introduction to Laplace Transform Techniques in Circuit Analysis Unit 6 Introduction to Laplace Tranform Technique in Circuit Analyi In thi unit we conider the application of Laplace Tranform to circuit analyi. A relevant dicuion of the one-ided Laplace tranform i found

More information

The Extended Balanced Truncation Algorithm

The Extended Balanced Truncation Algorithm International Journal of Coputing and Optiization Vol. 3, 2016, no. 1, 71-82 HIKARI Ltd, www.-hikari.co http://dx.doi.org/10.12988/ijco.2016.635 The Extended Balanced Truncation Algorith Cong Huu Nguyen

More information

Lecture 10 Filtering: Applied Concepts

Lecture 10 Filtering: Applied Concepts Lecture Filtering: Applied Concept In the previou two lecture, you have learned about finite-impule-repone (FIR) and infinite-impule-repone (IIR) filter. In thee lecture, we introduced the concept of filtering

More information

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

Lecture 36: MOSFET Common Drain (Source Follower) Amplifier. Whites, EE 320 Lecture 36 Pae 1 of 10 Lecture 36: MOSFET Coon Drain (Source Follower) Aplifier. The third, and last, discrete-for MOSFET aplifier we ll consider in this course is the coon drain aplifier.

More information

Lecture 12 - Non-isolated DC-DC Buck Converter

Lecture 12 - Non-isolated DC-DC Buck Converter ecture 12 - Non-iolated DC-DC Buck Converter Step-Down or Buck converter deliver DC power from a higher voltage DC level ( d ) to a lower load voltage o. d o ene ref + o v c Controller Figure 12.1 The

More information

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

Lecture 2 Phys 798S Spring 2016 Steven Anlage. The heart and soul of superconductivity is the Meissner Effect. This feature uniquely distinguishes ecture Phy 798S Spring 6 Steven Anlage The heart and oul of uperconductivity i the Meiner Effect. Thi feature uniquely ditinguihe uperconductivity fro any other tate of atter. Here we dicu oe iple phenoenological

More information

DIFFERENTIAL EQUATIONS

DIFFERENTIAL EQUATIONS Matheatic Reviion Guide Introduction to Differential Equation Page of Author: Mark Kudlowki MK HOME TUITION Matheatic Reviion Guide Level: A-Level Year DIFFERENTIAL EQUATIONS Verion : Date: 3-4-3 Matheatic

More information

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

Department of Mechanical Engineering Massachusetts Institute of Technology Modeling, Dynamics and Control III Spring 2002 Department of Mechanical Engineering Maachuett Intitute of Technology 2.010 Modeling, Dynamic and Control III Spring 2002 SOLUTIONS: Problem Set # 10 Problem 1 Etimating tranfer function from Bode Plot.

More information

Chapter 4. The Laplace Transform Method

Chapter 4. The Laplace Transform Method Chapter 4. The Laplace Tranform Method The Laplace Tranform i a tranformation, meaning that it change a function into a new function. Actually, it i a linear tranformation, becaue it convert a linear combination

More information

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

Lecture 4 Topic 3: General linear models (GLMs), the fundamentals of the analysis of variance (ANOVA), and completely randomized designs (CRDs) Lecture 4 Topic 3: General linear model (GLM), the fundamental of the analyi of variance (ANOVA), and completely randomized deign (CRD) The general linear model One population: An obervation i explained

More information

Design By Emulation (Indirect Method)

Design By Emulation (Indirect Method) Deign By Emulation (Indirect Method he baic trategy here i, that Given a continuou tranfer function, it i required to find the bet dicrete equivalent uch that the ignal produced by paing an input ignal

More information

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

Gain and Phase Margins Based Delay Dependent Stability Analysis of Two- Area LFC System with Communication Delays Gain and Phae Margin Baed Delay Dependent Stability Analyi of Two- Area LFC Sytem with Communication Delay Şahin Sönmez and Saffet Ayaun Department of Electrical Engineering, Niğde Ömer Halidemir Univerity,

More information

FUNDAMENTALS OF POWER SYSTEMS

FUNDAMENTALS OF POWER SYSTEMS 1 FUNDAMENTALS OF POWER SYSTEMS 1 Chapter FUNDAMENTALS OF POWER SYSTEMS INTRODUCTION The three baic element of electrical engineering are reitor, inductor and capacitor. The reitor conume ohmic or diipative

More information

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

If Y is normally Distributed, then and 2 Y Y 10. σ σ ull Hypothei Significance Teting V. APS 50 Lecture ote. B. Dudek. ot for General Ditribution. Cla Member Uage Only. Chi-Square and F-Ditribution, and Diperion Tet Recall from Chapter 4 material on: ( )

More information

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

SERIES COMPENSATION: VOLTAGE COMPENSATION USING DVR (Lectures 41-48) Chapter 5 SERIES COMPENSATION: VOLTAGE COMPENSATION USING DVR (Lecture 41-48) 5.1 Introduction Power ytem hould enure good quality of electric power upply, which mean voltage and current waveform hould

More information

7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281

7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281 72 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 28 and i 2 Show how Euler formula (page 33) can then be ued to deduce the reult a ( a) 2 b 2 {e at co bt} {e at in bt} b ( a) 2 b 2 5 Under what condition

More information

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

On the Use of High-Order Moment Matching to Approximate the Generalized-K Distribution by a Gamma Distribution On the Ue of High-Order Moent Matching to Approxiate the Generalized- Ditribution by a Gaa Ditribution Saad Al-Ahadi Departent of Syte & Coputer Engineering Carleton Univerity Ottawa Canada aahadi@ce.carleton.ca

More information

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

Chapter 7. Principles of Unsteady - State and Convective Mass Transfer Suppleental Material for Tranport Proce and Separation Proce Principle hapter 7 Principle of Unteady - State and onvective Ma Tranfer Thi chapter cover different ituation where a tranfer i taking place,

More information

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

Linearteam tech paper. The analysis of fourth-order state variable filter and it s application to Linkwitz- Riley filters Linearteam tech paper The analyi of fourth-order tate variable filter and it application to Linkwitz- iley filter Janne honen 5.. TBLE OF CONTENTS. NTOCTON.... FOTH-OE LNWTZ-LEY (L TNSFE FNCTON.... TNSFE

More information

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

SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuits II. Solutions to Assignment 3 February 2005. SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuit II Solution to Aignment 3 February 2005. Initial Condition Source 0 V battery witch flip at t 0 find i 3 (t) Component value:

More information

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

Image Denoising Based on Non-Local Low-Rank Dictionary Learning Advanced cience and Technology Letter Vol.11 (AT 16) pp.85-89 http://dx.doi.org/1.1457/atl.16. Iage Denoiing Baed on Non-Local Low-Rank Dictionary Learning Zhang Bo 1 1 Electronic and Inforation Engineering

More information

4 Conservation of Momentum

4 Conservation of Momentum hapter 4 oneration of oentu 4 oneration of oentu A coon itake inoling coneration of oentu crop up in the cae of totally inelatic colliion of two object, the kind of colliion in which the two colliding

More information

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

EE 508 Lecture 16. Filter Transformations. Lowpass to Bandpass Lowpass to Highpass Lowpass to Band-reject EE 508 Lecture 6 Filter Tranformation Lowpa to Bandpa Lowpa to Highpa Lowpa to Band-reject Review from Lat Time Theorem: If the perimeter variation and contact reitance are neglected, the tandard deviation

More information

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

Several schematic symbols for a capacitor are shown below. The symbol resembles the two conducting surfaces separated with a dielectric. Capacitor Capacitor are two terminal, paive energy torage device. They tore electrical potential energy in the form of an electric field or charge between two conducting urface eparated by an inulator

More information

AP Physics Momentum AP Wrapup

AP Physics Momentum AP Wrapup AP Phyic Moentu AP Wrapup There are two, and only two, equation that you get to play with: p Thi i the equation or oentu. J Ft p Thi i the equation or ipule. The equation heet ue, or oe reaon, the ybol

More information

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

Suggestions - Problem Set (a) Show the discriminant condition (1) takes the form. ln ln, # # R R Suggetion - Problem Set 3 4.2 (a) Show the dicriminant condition (1) take the form x D Ð.. Ñ. D.. D. ln ln, a deired. We then replace the quantitie. 3ß D3 by their etimate to get the proper form for thi

More information

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

Lecture 4. Chapter 11 Nise. Controller Design via Frequency Response. G. Hovland 2004 METR4200 Advanced Control Lecture 4 Chapter Nie Controller Deign via Frequency Repone G. Hovland 2004 Deign Goal Tranient repone via imple gain adjutment Cacade compenator to improve teady-tate error Cacade

More information

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

EE 508 Lecture 16. Filter Transformations. Lowpass to Bandpass Lowpass to Highpass Lowpass to Band-reject EE 508 Lecture 6 Filter Tranformation Lowpa to Bandpa Lowpa to Highpa Lowpa to Band-reject Review from Lat Time Theorem: If the perimeter variation and contact reitance are neglected, the tandard deviation

More information

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

SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuits II. R 4 := 100 kohm SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuit II Solution to Aignment 3 February 2003. Cacaded Op Amp [DC&L, problem 4.29] An ideal op amp ha an output impedance of zero,

More information

Chapter 10 Transistor amplifier design

Chapter 10 Transistor amplifier design hapter 0 Tranitor amplifier dein 0. tability conideration unconditionally table conditionally table tability factor ource tability circle load tability circle 0. mplifier dein for maximum ain unilateral

More information

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

Lecture 10 OUTLINE. Reading: Chapter EE105 Spring 2008 Lecture 10, Slide 1 Prof. Wu, UC Berkeley Lecture 0 OUTLIN BJT Aplifiers (3) itter follower (Coon-collector aplifier) Analysis of eitter follower core Ipact of source resistance Ipact of arly effect itter follower with biasin eadin: Chapter 5.3.3-5.4

More information

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

Fig.L3.1. A cross section of a MESFET (a) and photograph and electrode layout (b). ECEN 5004, Sprin 2018 Active Microwave Circuit Zoya Popovic, Univerity of Colorado, Boulder LECURE 3 MICROWAVE RANSISOR OVERVIEW AND RANSISOR EQUIVALEN CIRCUIS L3.1. MESFES AND HEMS he ot coonly ued active

More information

Lecture #9 Continuous time filter

Lecture #9 Continuous time filter Lecture #9 Continuou time filter Oliver Faut December 5, 2006 Content Review. Motivation......................................... 2 2 Filter pecification 2 2. Low pa..........................................

More information

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

into a discrete time function. Recall that the table of Laplace/z-transforms is constructed by (i) selecting to get Lecture 25 Introduction to Some Matlab c2d Code in Relation to Sampled Sytem here are many way to convert a continuou time function, { h( t) ; t [0, )} into a dicrete time function { h ( k) ; k {0,,, }}

More information

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

Chapter 5 Consistency, Zero Stability, and the Dahlquist Equivalence Theorem Chapter 5 Conitency, Zero Stability, and the Dahlquit Equivalence Theorem In Chapter 2 we dicued convergence of numerical method and gave an experimental method for finding the rate of convergence (aka,

More information

Tuning of High-Power Antenna Resonances by Appropriately Reactive Sources

Tuning of High-Power Antenna Resonances by Appropriately Reactive Sources Senor and Simulation Note Note 50 Augut 005 Tuning of High-Power Antenna Reonance by Appropriately Reactive Source Carl E. Baum Univerity of New Mexico Department of Electrical and Computer Engineering

More information

Highway Capacity Manual 2010

Highway Capacity Manual 2010 RR = minimum number of lane change that mut be made by one ramp-toramp ehicle to execute the deired maneuer uccefully. MIN for two-ided weaing egment i gien by Equation 12-3: MIN RR For two-ided weaing

More information

online learning Unit Workbook 4 RLC Transients

online learning Unit Workbook 4 RLC Transients online learning Pearon BTC Higher National in lectrical and lectronic ngineering (QCF) Unit 5: lectrical & lectronic Principle Unit Workbook 4 in a erie of 4 for thi unit Learning Outcome: RLC Tranient

More information

PHYSICS 151 Notes for Online Lecture 2.3

PHYSICS 151 Notes for Online Lecture 2.3 PHYSICS 151 Note for Online Lecture.3 riction: The baic fact of acrocopic (everda) friction are: 1) rictional force depend on the two aterial that are liding pat each other. bo liding over a waed floor

More information

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

11.2 Stability. A gain element is an active device. One potential problem with every active circuit is its stability 5/7/2007 11_2 tability 1/2 112 tability eading Aignment: pp 542-548 A gain element i an active device One potential problem with every active circuit i it tability HO: TABIITY Jim tile The Univ of Kana

More information

Section Induction motor drives

Section Induction motor drives Section 5.1 - nduction motor drive Electric Drive Sytem 5.1.1. ntroduction he AC induction motor i by far the mot widely ued motor in the indutry. raditionally, it ha been ued in contant and lowly variable-peed

More information

Frequency Response of Amplifiers

Frequency Response of Amplifiers 類比電路設計 (3349-004 Frequency epne f Aplifier h-uan an Natinal hun-h Univerity epartent f Electrical Eneer Overview ead B azavi hapter 6 ntrductin n thi lecture, we tudy the repne f le-tae and differential

More information

Social Studies 201 Notes for March 18, 2005

Social Studies 201 Notes for March 18, 2005 1 Social Studie 201 Note for March 18, 2005 Etimation of a mean, mall ample ize Section 8.4, p. 501. When a reearcher ha only a mall ample ize available, the central limit theorem doe not apply to the

More information

The Electric Potential Energy

The Electric Potential Energy Lecture 6 Chapter 28 Phyic II The Electric Potential Energy Coure webite: http://aculty.uml.edu/andriy_danylov/teaching/phyicii New Idea So ar, we ued vector quantitie: 1. Electric Force (F) Depreed! 2.

More information

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

UNIT 15 RELIABILITY EVALUATION OF k-out-of-n AND STANDBY SYSTEMS UNIT 1 RELIABILITY EVALUATION OF k-out-of-n AND STANDBY SYSTEMS Structure 1.1 Introduction Objective 1.2 Redundancy 1.3 Reliability of k-out-of-n Sytem 1.4 Reliability of Standby Sytem 1. Summary 1.6 Solution/Anwer

More information

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

ECE 3510 Root Locus Design Examples. PI To eliminate steady-state error (for constant inputs) & perfect rejection of constant disturbances ECE 350 Root Locu Deign Example Recall the imple crude ervo from lab G( ) 0 6.64 53.78 σ = = 3 23.473 PI To eliminate teady-tate error (for contant input) & perfect reection of contant diturbance Note:

More information

ADAPTIVE CONTROL DESIGN FOR A SYNCHRONOUS GENERATOR

ADAPTIVE CONTROL DESIGN FOR A SYNCHRONOUS GENERATOR ADAPTIVE CONTROL DESIGN FOR A SYNCHRONOUS GENERATOR SAEED ABAZARI MOHSEN HEIDARI NAVID REZA ABJADI Key word: Adaptive control Lyapunov tability Tranient tability Mechanical power. The operating point of

More information

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

s s 1 s = m s 2 = 0; Δt = 1.75s; a =? mi hr Flipping Phyic Lecture Note: Introduction to Acceleration with Priu Brake Slaing Exaple Proble a Δv a Δv v f v i & a t f t i Acceleration: & flip the guy and ultiply! Acceleration, jut like Diplaceent

More information

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

NOTE: The items d) and e) of Question 4 gave you bonus marks. MAE 40 Linear ircuit Summer 2007 Final Solution NOTE: The item d) and e) of Quetion 4 gave you bonu mark. Quetion [Equivalent irciut] [4 mark] Find the equivalent impedance between terminal A and B in

More information

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

EE 4443/5329. LAB 3: Control of Industrial Systems. Simulation and Hardware Control (PID Design) The Inverted Pendulum. (ECP Systems-Model: 505) EE 4443/5329 LAB 3: Control of Indutrial Sytem Simulation and Hardware Control (PID Deign) The Inverted Pendulum (ECP Sytem-Model: 505) Compiled by: Nitin Swamy Email: nwamy@lakehore.uta.edu Email: okuljaca@lakehore.uta.edu

More information

Per Unit Analysis. Single-Phase systems

Per Unit Analysis. Single-Phase systems Per Unit Analyi The per unit method of power ytem analyi eliminate the need for converion of voltae, current and impedance acro every tranformer in the circuit. n addition, the need to tranform from 3-

More information

Physics 20 Lesson 16 Friction

Physics 20 Lesson 16 Friction Phyic 0 Leon 16 riction In the previou leon we learned that a rictional orce i any orce that reit, retard or ipede the otion o an object. In thi leon we will dicu how riction reult ro the contact between

More information

Kalman Filter. Wim van Drongelen, Introduction

Kalman Filter. Wim van Drongelen, Introduction alman Filter Wim an Drongelen alman Filter Wim an Drongelen, 03. Introduction Getting to undertand a ytem can be quite a challenge. One approach i to create a model, an abtraction of the ytem. The idea

More information

Clustering Methods without Given Number of Clusters

Clustering Methods without Given Number of Clusters Clutering Method without Given Number of Cluter Peng Xu, Fei Liu Introduction A we now, mean method i a very effective algorithm of clutering. It mot powerful feature i the calability and implicity. However,

More information

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

EECS240 Spring Lecture 13: Settling. Lingkai Kong Dept. of EECS EES240 Spring 203 Lecture 3: Settling Lingkai Kong Dept. of EES Settling Why intereted in ettling? Ocillocope: track input waveform without ringing AD (witchedcap amplifier): gain a ignal up by a precie

More information

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

Part A: Signal Processing. Professor E. Ambikairajah UNSW, Australia Part A: Signal Proceing Chapter 5: Digital Filter Deign 5. Chooing between FIR and IIR filter 5. Deign Technique 5.3 IIR filter Deign 5.3. Impule Invariant Method 5.3. Bilinear Tranformation 5.3.3 Digital

More information

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

Module 4: Time Response of discrete time systems Lecture Note 1 Digital Control Module 4 Lecture Module 4: ime Repone of dicrete time ytem Lecture Note ime Repone of dicrete time ytem Abolute tability i a baic requirement of all control ytem. Apart from that, good

More information

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

Chapter 2 Sampling and Quantization. In order to investigate sampling and quantization, the difference between analog Chapter Sampling and Quantization.1 Analog and Digital Signal In order to invetigate ampling and quantization, the difference between analog and digital ignal mut be undertood. Analog ignal conit of continuou

More information

Name: Answer Key Date: Regents Physics. Energy

Name: Answer Key Date: Regents Physics. Energy Nae: Anwer Key Date: Regent Phyic Tet # 9 Review Energy 1. Ue GUESS ethod and indicate all vector direction.. Ter to know: work, power, energy, conervation of energy, work-energy theore, elatic potential

More information

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

Zbigniew Dziong Department of Electrical Engineering, Ecole de Technologie Superieure 1100 Notre-Dame Street West, Montreal, Quebec, Canada H3C 1k3 Capacity Allocation in Serice Oerlay Network - Maximum Profit Minimum Cot Formulation Ngok Lam Department of Electrical and Computer Engineering, McGill Unierity 3480 Unierity Street, Montreal, Quebec,

More information

CHAPTER 5. The Operational Amplifier 1

CHAPTER 5. The Operational Amplifier 1 EECE22 NETWORK ANALYSIS I Dr. Charle J. Kim Cla Note 9: Oerational Amlifier (OP Am) CHAPTER. The Oerational Amlifier A. INTRODUCTION. The oerational amlifier or o am for hort, i a eratile circuit building

More information

Nonlinear Single-Particle Dynamics in High Energy Accelerators

Nonlinear Single-Particle Dynamics in High Energy Accelerators Nonlinear Single-Particle Dynamic in High Energy Accelerator Part 6: Canonical Perturbation Theory Nonlinear Single-Particle Dynamic in High Energy Accelerator Thi coure conit of eight lecture: 1. Introduction

More information

12.4 Atomic Absorption and Emission Spectra

12.4 Atomic Absorption and Emission Spectra Phyic Tool box 12.4 Atoic Abortion and iion Sectra A continuou ectru given off by a heated olid i caued by the interaction between neighbouring ato or olecule. An eiion ectru or line ectru i eitted fro

More information

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

Given the following circuit with unknown initial capacitor voltage v(0): X(s) Immediately, we know that the transfer function H(s) is EE 4G Note: Chapter 6 Intructor: Cheung More about ZSR and ZIR. Finding unknown initial condition: Given the following circuit with unknown initial capacitor voltage v0: F v0/ / Input xt 0Ω Output yt -

More information

Preemptive scheduling on a small number of hierarchical machines

Preemptive scheduling on a small number of hierarchical machines Available online at www.ciencedirect.com Information and Computation 06 (008) 60 619 www.elevier.com/locate/ic Preemptive cheduling on a mall number of hierarchical machine György Dóa a, Leah Eptein b,

More information

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 =

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 = Our online Tutor are available 4*7 to provide Help with Proce control ytem Homework/Aignment or a long term Graduate/Undergraduate Proce control ytem Project. Our Tutor being experienced and proficient

More information

THE BICYCLE RACE ALBERT SCHUELLER

THE BICYCLE RACE ALBERT SCHUELLER THE BICYCLE RACE ALBERT SCHUELLER. INTRODUCTION We will conider the ituation of a cyclit paing a refrehent tation in a bicycle race and the relative poition of the cyclit and her chaing upport car. The

More information

Improving the Efficiency of a Digital Filtering Scheme for Diabatic Initialization

Improving the Efficiency of a Digital Filtering Scheme for Diabatic Initialization 1976 MONTHLY WEATHER REVIEW VOLUME 15 Improving the Efficiency of a Digital Filtering Scheme for Diabatic Initialization PETER LYNCH Met Éireann, Dublin, Ireland DOMINIQUE GIARD CNRM/GMAP, Météo-France,

More information

HOMEWORK ASSIGNMENT #2

HOMEWORK ASSIGNMENT #2 Texa A&M Univerity Electrical Engineering Department ELEN Integrated Active Filter Deign Methodologie Alberto Valde-Garcia TAMU ID# 000 17 September 0, 001 HOMEWORK ASSIGNMENT # PROBLEM 1 Obtain at leat

More information

CHAPTER 14 SIGNAL GENERATORS AND WAVEFORM-SHAPING CIRCUITS

CHAPTER 14 SIGNAL GENERATORS AND WAVEFORM-SHAPING CIRCUITS CHAPTE 4 SIGNA GENEATS AN WAEFM-SHAPING CICUITS Chapter utline 4. Baic Principle o Sinuoidal cillator 4. p Amp-C cillator 4. C and Crytal cillator 4.4 Bitable Multiibrator 4.5 Generation o Square and Triangular

More information

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

Source slideplayer.com/fundamentals of Analytical Chemistry, F.J. Holler, S.R.Crouch. Chapter 6: Random Errors in Chemical Analysis Source lideplayer.com/fundamental of Analytical Chemitry, F.J. Holler, S.R.Crouch Chapter 6: Random Error in Chemical Analyi Random error are preent in every meaurement no matter how careful the experimenter.

More information

5.5 Application of Frequency Response: Signal Filters

5.5 Application of Frequency Response: Signal Filters 44 Dynamic Sytem Second order lowpa filter having tranfer function H()=H ()H () u H () H () y Firt order lowpa filter Figure 5.5: Contruction of a econd order low-pa filter by combining two firt order

More information

Linear Motion, Speed & Velocity

Linear Motion, Speed & Velocity Add Important Linear Motion, Speed & Velocity Page: 136 Linear Motion, Speed & Velocity NGSS Standard: N/A MA Curriculum Framework (006): 1.1, 1. AP Phyic 1 Learning Objective: 3.A.1.1, 3.A.1.3 Knowledge/Undertanding

More information

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

A Full-Newton Step Primal-Dual Interior Point Algorithm for Linear Complementarity Problems * ISSN 76-7659, England, UK Journal of Information and Computing Science Vol 5, No,, pp 35-33 A Full-Newton Step Primal-Dual Interior Point Algorithm for Linear Complementarity Problem * Lipu Zhang and Yinghong

More information

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

What lies between Δx E, which represents the steam valve, and ΔP M, which is the mechanical power into the synchronous machine? A 2.0 Introduction In the lat et of note, we developed a model of the peed governing mechanim, which i given below: xˆ K ( Pˆ ˆ) E () In thee note, we want to extend thi model o that it relate the actual

More information

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

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 Chapter Homework Solution P.-1,, 5 P.4-1, 3, 5, 6, 7 P.5-1, 3, 5 P.6-, 5 P.7-1, 4 P.8-1 P.9-1 P.-1 An element ha oltage and current i a hown in Figure P.-1a. Value of the current i and correponding oltage

More information

Publication V by authors

Publication V by authors Publication Kontantin S. Kotov and Jorma J. Kyyrä. 008. nertion lo and network parameter in the analyi of power filter. n: Proceeding of the 008 Nordic Workhop on Power and ndutrial Electronic (NORPE 008).

More information

CISE302: Linear Control Systems

CISE302: Linear Control Systems Term 8 CISE: Linear Control Sytem Dr. Samir Al-Amer Chapter 7: Root locu CISE_ch 7 Al-Amer8 ١ Learning Objective Undertand the concept of root locu and it role in control ytem deign Be able to ketch root

More information

Chapter 7. Root Locus Analysis

Chapter 7. Root Locus Analysis Chapter 7 Root Locu Analyi jw + KGH ( ) GH ( ) - K 0 z O 4 p 2 p 3 p Root Locu Analyi The root of the cloed-loop characteritic equation define the ytem characteritic repone. Their location in the complex

More information