General Topology of a single stage microwave amplifier

Size: px
Start display at page:

Download "General Topology of a single stage microwave amplifier"

Transcription

1 General Topology of a ingle tage microwave amplifier Tak of MATCH network (in and out): To preent at the active device uitable impedance Z and Z S Deign Step The deign of a mall ignal microwave amplifier at a ingle frequency i compoed of the following tep: Choice of active device Evaluation of optimum load for the device (Z and Z S ) Synthei of MATCH network

2 Active device repreentation The active device i repreented by mean of it meaured cattering parameter in the pecified bia condition. The reference impedance i typically 50 Ohm S v in S (50Ω) S Z Z Z Z S S Uing uitable formula, it i poible to evaluate the Tranducer Gain and the reflection coefficient at input and output.

3 Evaluation of in, out and G T S (50Ω) All reflection coefficient are defined with repect 50 Ω: in out ZS 50 Z 50 S, Z + 50 Z + 50 S in Z Z in in ( ) 1 1 Z out 50 + out Z out + 50 ( 1 S ) S 1 1 G T (1 S ) (1 ) 1 (1 ) (1 ) S S 1 1

4 Stability Iue A -port network operating a an amplifier mut be table, i.e. the output ignal mut remain of finite amplitude for an input exciting ignal with finite amplitude A -port i aid unconditionally table if, for whatever value of e S, it ha: S S in out 1 1 in + < S out + < 1 S 1 1 If both the condition are not atified the -port i aid potentially intable

5 Stability Condition Given the S parameter, the condition in <1, out <1 are verified for whatever value of S, if: K > 1, Det S 1 1 [ ] < 1 When thee equation are verified (and the port i unconditionally table ) a pair S,opt,,opt doe exit which determine the conjugate matching both at input and output. In thi condition G T i maximum and can be expreed a: G 1, T MAX 1 ( K K ) 1

6 B C g g 1 + Expreion for S,opt,,opt C B B C 1 ( 4 ) * g g g g S, opt C ( 4 ) C B B C C 1 *, opt * ( ) C ( ) g B * 1 1 NOTE: The above equation hold for 1 0. They are the olution of the ytem:, opt * 1 1, opt ( ) +, ( ) in * * 1 1 S, opt, + 1, 1 opt out opt S, opt *

7 Potentially Intable Device When k<1 a pair ( S, ) doe not exit for which G T i maximum. In cae of intability G T become in fact infinity. The admiible value of S, mut however atify the condition + < + < in S 1, out S Thee contraint, reported graphically on the Smith Chart, allow to identify the admiible value of di S e. A a guideline for the choice of G T the maximum table gain can be G conidered: T,max The elected value of G T hould be maller of thi value. 1 1

8 Admiible region for S The equation defining the boundary of thi region i: 1 1 S out + 1 S The equation define a circle with centre and radiu given by: 1 C S * * C r r 1 1 Plane S

9 Admiible region per The equation defining the boundary of thi region i: 1 1 in + 1 The equation define a circle with centre and radiu given by: 1 C * * C r r 1 1 Plane

10 Identification of admiible region The circle een in the previou lide define the boundary between the admiible and not admiible region. To identify which of the two i the table region the value of in ( out ) for ( S )0 mut be oberved. Taking into account that in ( out ) coincide in thi cae with ( ), it ha: The table region for ( S ) i outide the intability circle if: - ( ) <1 and the circle doe not encloe the centre of the chart - ( ) >1 and the circle encloe the centre of the chart The table region for ( S ) i inide the intability circle if : - ( ) >1 and the circle doe not encloe the centre of the chart - ( ) <1 and the circle encloe the centre of the chart

11 Amplifier deign with potentially intable device In thi cae there i not a unique olution. It i however poible: To choice in the table region and compute S for the maximum G T (alo the reulting S mut be inide the table region) To choice S in the table region and compute for the maximum G T (alo the reulting mut be inide the table region) To maximize G T the conjugate matching condition mut be impoed, i.e: ( ) in * * Cae 1 ( ) out * S 1 S * Cae

12 Circle with contant G p From the definition of Power Gain G p the following expreion i derived: G p (1 ) ( ) ( ) 1 * 1 + Re Note that G p doe not depend on S. Moreover it alway larger than or equal to G T ; it i equal when the input i matched: in ( ) *. Drawing the previou equation in the plane, we found a curve on thi plane where G p i contant; thi curve i a circle with the following center and radiu (g p G p / 1 ): C p * * ( ) ( ) ( ) 1 k gp + gp ( ) p gp, r 1+ g 1+ g p p 1

13 Deign with aigned G p Select an active device with the requeted G T (maximum table gain) Draw the circle G p G T on the Smith Chart repreenting Select a point on thi circle in the table region; thi i the elected,opt Compute S,opt by impoing the matching at the input. Verify that alo S,opt i in the table region of S., opt + 1 1, opt 1, opt Note: Once S,opt i aigned to the ource, the input i matched and, a a conequence, the tranducer power gain coincide numerically with the impoed power gain * S,opt Intability region of the ource Circle G p cot,opt Intability region of the load

14 Circle with contant G a From the definition of Available Power Gain G a the following expreion i derived : G a (1 ) ( ) S ( ) 1 * 1 +S Re S Note that G a doe not depend on. Moreover it alway larger than or equal to G T ; it i equal when the output i matched: out ( ) *. Drawing the previou equation in the plane S, we found a curve on thi plane where G a i contant; thi curve i a circle with the following center and radiu (g a G a / 1 ): C a a * * ( ) g, r ( ) ( ) 1 k ga + ga ( ) a a 1+ g 1+ g a 1

15 Deign with aigned Gp Select an active device with the requeted G T (maximum table gain) Draw the circle G a G T on the Smith Chart repreenting S Select a point on thi circle in the table region; thi i the elected S,opt Compute,opt by impoing the matching at output. Verify that alo,opt i in the table region of., opt S, opt 1 S, opt Note: Once,opt i aigned to the load, the output i matched and, a a conequence, the tranducer power gain coincide numerically with the impoed available power gain *,opt Intability region of the load Cerchio a G a cot S,opt Intability region of the ource

16 Deign reult Once the value of,opt and S,opt have been obtained with once of the method preented, we have: Cae 1 (Aigned Gp) Traduced Gain impoed Input Matched (NOT the output) Cae (Aigned Ga) Traduced Gain impoed Output Matched (NOT the input) NOTE: If lole network are ued for realized,opt and S,opt, alo the input or the output of the amplifier i matched

17 Example: Deign of a 1 GHz Amplifier Active device NEC70000 (GaA Mefet ) Max Gain at 1 GHz: 13.4 db Amplifier requirement Frequency band: GHz Tranducer gain in band: 1.5 ± 0.5 db Output Matching: < -15 db Topology: Subtrate ε r 9.8 H 0.6 mm t 50 µm Rho (reitivity normalized to Gold) 1 50 Ω In Out 50 Ω V in out

18 Biaing network of the active device V GS Bia V DS Bia RF Short Circuit RF Open Circuit NOTE: The S parameter delivered by the manufacturer refer to the red ection. After the biaing network ha been aigned, the S parameter change to the one referred to the black ection Input reference ection Block Capacitor (DC) Output reference ection

19 Scattering parameter of the biaed tranitor S parameter at 1 GHz S (Mag, Phae deg) 0.704, S1 (Mag, Phae deg) 0.099, -5.7 S1 (Mag, Phae deg).067, S (Mag, Phae deg) 0.467, Stability Coefficient: Potentially Intable K 1 S S + SS S1S1 < S S Maximum Stable Gain (db): S S 1 10 log

20 Evaluation of and S Aigned Ga : 1.5 db Choice of S Evaluation of ( out ) * Matching network (ingle tub topology) X

21 Input Network TIN E1.9 Deg F01.e4 MHz PORT RES R50 Ohm TSC E35.54 Deg F01.e4 MHz S ine : Φ β 1.91 Stub admittance: j B -j.475 -j cotan(β S ) Stub length (.c.) : Φ S tan

22 Output Network TIN E131.6 Deg F01.e4 MHz PORT RES R50 Ohm TSC E4.51 Deg F01.e4 MHz ine : Φ β Stub admittance: j B -j.193 -j cotan(β S ) Stub length (.c.) : 1 1 Φ S tan

23 Simulated repone 14 Ampli Initial Repone S S S DB( S(1,1) ) (R) Ampli Ottimizzato DB( S(,1) ) () Ampli Ottimizzato DB( S(,) ) (R) Ampli Ottimizzato Frequency (MHz) PORT P1 Z50 Ohm TIN IDT1 Z050 Ohm EFI1 Deg F0f0 MHz SUBCKT IDS1 NET"nec7000pola" 1 TIN IDT Z050 Ohm EFI3 Deg F0f0 MHz PORT P Z50 Ohm TSC IDT3 Z050 Ohm EFI Deg F0f0 MHz TSC IDT4 Z050 Ohm EFI4 Deg F0f0 MHz

24 Optimized Repone Ampli Optimized Repone S S S DB( S(1,1) ) (R) Ampli Ottimizzato DB( S(,1) ) () Ampli Ottimizzato DB( S(,) ) (R) Ampli Ottimizzato Frequency (MHz)

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

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

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

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

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

The Measurement of DC Voltage Signal Using the UTI

The Measurement of DC Voltage Signal Using the UTI he Meaurement of DC Voltage Signal Uing the. INRODUCION can er an interface for many paive ening element, uch a, capacitor, reitor, reitive bridge and reitive potentiometer. By uing ome eternal component,

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

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

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

NAME (pinyin/italian)... MATRICULATION NUMBER... SIGNATURE

NAME (pinyin/italian)... MATRICULATION NUMBER... SIGNATURE POLITONG SHANGHAI BASIC AUTOMATIC CONTROL June Academic Year / Exam grade NAME (pinyin/italian)... MATRICULATION NUMBER... SIGNATURE Ue only thee page (including the bac) for anwer. Do not ue additional

More information

Chapter 9: Controller design. Controller design. Controller design

Chapter 9: Controller design. Controller design. Controller design Chapter 9. Controller Deign 9.. Introduction 9.2. Eect o negative eedback on the network traner unction 9.2.. Feedback reduce the traner unction rom diturbance to the output 9.2.2. Feedback caue the traner

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

III.9. THE HYSTERESIS CYCLE OF FERROELECTRIC SUBSTANCES

III.9. THE HYSTERESIS CYCLE OF FERROELECTRIC SUBSTANCES III.9. THE HYSTERESIS CYCLE OF FERROELECTRIC SBSTANCES. Work purpoe The analyi of the behaviour of a ferroelectric ubtance placed in an eternal electric field; the dependence of the electrical polariation

More information

Bogoliubov Transformation in Classical Mechanics

Bogoliubov Transformation in Classical Mechanics Bogoliubov Tranformation in Claical Mechanic Canonical Tranformation Suppoe we have a et of complex canonical variable, {a j }, and would like to conider another et of variable, {b }, b b ({a j }). How

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

Microwave Oscillators Design

Microwave Oscillators Design Microwave Oscillators Design Oscillators Classification Feedback Oscillators β Α Oscillation Condition: Gloop = A β(jω 0 ) = 1 Gloop(jω 0 ) = 1, Gloop(jω 0 )=2nπ Negative resistance oscillators Most used

More information

ME 375 FINAL EXAM Wednesday, May 6, 2009

ME 375 FINAL EXAM Wednesday, May 6, 2009 ME 375 FINAL EXAM Wedneday, May 6, 9 Diviion Meckl :3 / Adam :3 (circle one) Name_ Intruction () Thi i a cloed book examination, but you are allowed three ingle-ided 8.5 crib heet. A calculator i NOT allowed.

More information

A Simple Approach to Synthesizing Naïve Quantized Control for Reference Tracking

A Simple Approach to Synthesizing Naïve Quantized Control for Reference Tracking A Simple Approach to Syntheizing Naïve Quantized Control for Reference Tracking SHIANG-HUA YU Department of Electrical Engineering National Sun Yat-Sen Univerity 70 Lien-Hai Road, Kaohiung 804 TAIAN Abtract:

More information

Example: Amplifier Distortion

Example: Amplifier Distortion 4/6/2011 Example Amplifier Ditortion 1/9 Example: Amplifier Ditortion Recall thi circuit from a previou handout: 15.0 R C =5 K v ( t) = v ( t) o R B =5 K β = 100 _ vi( t ) 58. R E =5 K CUS We found that

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

Root Locus Diagram. Root loci: The portion of root locus when k assume positive values: that is 0

Root Locus Diagram. Root loci: The portion of root locus when k assume positive values: that is 0 Objective Root Locu Diagram Upon completion of thi chapter you will be able to: Plot the Root Locu for a given Tranfer Function by varying gain of the ytem, Analye the tability of the ytem from the root

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

HIGHER-ORDER FILTERS. Cascade of Biquad Filters. Follow the Leader Feedback Filters (FLF) ELEN 622 (ESS)

HIGHER-ORDER FILTERS. Cascade of Biquad Filters. Follow the Leader Feedback Filters (FLF) ELEN 622 (ESS) HIGHER-ORDER FILTERS Cacade of Biquad Filter Follow the Leader Feedbac Filter (FLF) ELEN 6 (ESS) Than for ome of the material to David Hernandez Garduño CASCADE FILTER DESIGN N H ( ) Π H ( ) H ( ) H (

More information

CHAPTER 4 DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL

CHAPTER 4 DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL 98 CHAPTER DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL INTRODUCTION The deign of ytem uing tate pace model for the deign i called a modern control deign and it i

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

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

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

ECE-202 FINAL December 13, 2016 CIRCLE YOUR DIVISION

ECE-202 FINAL December 13, 2016 CIRCLE YOUR DIVISION ECE-202 Final, Fall 16 1 ECE-202 FINAL December 13, 2016 Name: (Pleae print clearly.) Student Email: CIRCLE YOUR DIVISION DeCarlo- 8:30-9:30 Talavage-9:30-10:30 2021 2022 INSTRUCTIONS There are 35 multiple

More information

EE105 - Fall 2005 Microelectronic Devices and Circuits

EE105 - Fall 2005 Microelectronic Devices and Circuits EE5 - Fall 5 Microelectronic Device and ircuit Lecture 9 Second-Order ircuit Amplifier Frequency Repone Announcement Homework 8 due tomorrow noon Lab 7 next week Reading: hapter.,.3. Lecture Material Lat

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

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

Noise Figure Minimization of RC Polyphase Filters

Noise Figure Minimization of RC Polyphase Filters Noie Figure Mimization of olyphae Filter Jáno advánzky Abtract - ideband uppreion of polyphae filter i dependent of the ource and load impedance. Thi property i valid for any number of tage and any detung

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

CONTROL SYSTEMS, ROBOTICS AND AUTOMATION Vol. VIII Decoupling Control - M. Fikar

CONTROL SYSTEMS, ROBOTICS AND AUTOMATION Vol. VIII Decoupling Control - M. Fikar DECOUPLING CONTROL M. Fikar Department of Proce Control, Faculty of Chemical and Food Technology, Slovak Univerity of Technology in Bratilava, Radlinkého 9, SK-812 37 Bratilava, Slovakia Keyword: Decoupling:

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

Digital Control System

Digital Control System Digital Control Sytem - A D D A Micro ADC DAC Proceor Correction Element Proce Clock Meaurement A: Analog D: Digital Continuou Controller and Digital Control Rt - c Plant yt Continuou Controller Digital

More information

CHEAP CONTROL PERFORMANCE LIMITATIONS OF INPUT CONSTRAINED LINEAR SYSTEMS

CHEAP CONTROL PERFORMANCE LIMITATIONS OF INPUT CONSTRAINED LINEAR SYSTEMS Copyright 22 IFAC 5th Triennial World Congre, Barcelona, Spain CHEAP CONTROL PERFORMANCE LIMITATIONS OF INPUT CONSTRAINED LINEAR SYSTEMS Tritan Pérez Graham C. Goodwin Maria M. Serón Department of Electrical

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

Emittance limitations due to collective effects for the TOTEM beams

Emittance limitations due to collective effects for the TOTEM beams LHC Project ote 45 June 0, 004 Elia.Metral@cern.ch Andre.Verdier@cern.ch Emittance limitation due to collective effect for the TOTEM beam E. Métral and A. Verdier, AB-ABP, CER Keyword: TOTEM, collective

More information

ISSN: ISO 9001:2008 Certified International Journal of Engineering and Innovative Technology (IJEIT) Volume 5, Issue 5, November 2015

ISSN: ISO 9001:2008 Certified International Journal of Engineering and Innovative Technology (IJEIT) Volume 5, Issue 5, November 2015 Optimum Deign of Charge Pump Circuit Uing Genetic Algorithm Dr. Ahmad T. Youni, Shamil H. Huein, and Ahmad A. Imail Abtract Integrated charge pump circuit are power converter ued to obtain a different

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

Follow The Leader Architecture

Follow The Leader Architecture ECE 6(ESS) Follow The Leader Architecture 6 th Order Elliptic andpa Filter A numerical example Objective To deign a 6th order bandpa elliptic filter uing the Follow-the-Leader (FLF) architecture. The pecification

More information

Comparison of Hardware Tests with SIMULINK Models of UW Microgrid

Comparison of Hardware Tests with SIMULINK Models of UW Microgrid Comparion of Hardware Tet with SIMULINK Model of UW Microgrid Introduction Thi report include a detailed dicuion of the microource available on the Univerity- of- Wiconin microgrid. Thi include detail

More information

Analysis of Prevention of Induction Motors Stalling by Capacitor Switching

Analysis of Prevention of Induction Motors Stalling by Capacitor Switching 16th NTIONL POWER SYSTEMS CONFERENCE, 15th-17th DECEMER, 2010 260 nalyi of Prevention of Induction Motor Stalling by Capacitor Switching S.Maheh and P.S Nagendra rao Department of Electrical Engineering

More information

Automatic Control Systems. Part III: Root Locus Technique

Automatic Control Systems. Part III: Root Locus Technique www.pdhcenter.com PDH Coure E40 www.pdhonline.org Automatic Control Sytem Part III: Root Locu Technique By Shih-Min Hu, Ph.D., P.E. Page of 30 www.pdhcenter.com PDH Coure E40 www.pdhonline.org VI. Root

More information

Lecture 8. PID control. Industrial process control ( today) PID control. Insights about PID actions

Lecture 8. PID control. Industrial process control ( today) PID control. Insights about PID actions Lecture 8. PID control. The role of P, I, and D action 2. PID tuning Indutrial proce control (92... today) Feedback control i ued to improve the proce performance: tatic performance: for contant reference,

More information

Design of Digital Filters

Design of Digital Filters Deign of Digital Filter Paley-Wiener Theorem [ ] ( ) If h n i a caual energy ignal, then ln H e dω< B where B i a finite upper bound. One implication of the Paley-Wiener theorem i that a tranfer function

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

Designing Circuits Synthesis - Lego

Designing Circuits Synthesis - Lego Deigning Circuit Synthei Lego Port a pair of terminal to a cct Oneport cct; meaure I and at ame port I Drivingpoint impedance input impedance equiv impedance Twoport Tranfer function; meaure input at one

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

EE/ME/AE324: Dynamical Systems. Chapter 8: Transfer Function Analysis

EE/ME/AE324: Dynamical Systems. Chapter 8: Transfer Function Analysis EE/ME/AE34: Dynamical Sytem Chapter 8: Tranfer Function Analyi The Sytem Tranfer Function Conider the ytem decribed by the nth-order I/O eqn.: ( n) ( n 1) ( m) y + a y + + a y = b u + + bu n 1 0 m 0 Taking

More information

R. W. Erickson. Department of Electrical, Computer, and Energy Engineering University of Colorado, Boulder

R. W. Erickson. Department of Electrical, Computer, and Energy Engineering University of Colorado, Boulder R. W. Erickon Department of Electrical, Computer, and Energy Engineering Univerity of Colorado, Boulder Cloed-loop buck converter example: Section 9.5.4 In ECEN 5797, we ued the CCM mall ignal model to

More information

These are practice problems for the final exam. You should attempt all of them, but turn in only the even-numbered problems!

These are practice problems for the final exam. You should attempt all of them, but turn in only the even-numbered problems! Math 33 - ODE Due: 7 December 208 Written Problem Set # 4 Thee are practice problem for the final exam. You hould attempt all of them, but turn in only the even-numbered problem! Exercie Solve the initial

More information

Multivariable Control Systems

Multivariable Control Systems Lecture Multivariable Control Sytem Ali Karimpour Aociate Profeor Ferdowi Univerity of Mahhad Lecture Reference are appeared in the lat lide. Dr. Ali Karimpour May 6 Uncertainty in Multivariable Sytem

More information

Reference:W:\Lib\MathCAD\Default\defaults.mcd

Reference:W:\Lib\MathCAD\Default\defaults.mcd 4/9/9 Page of 5 Reference:W:\Lib\MathCAD\Default\default.mcd. Objective a. Motivation. Finite circuit peed, e.g. amplifier - effect on ignal. E.g. how "fat" an amp do we need for audio? For video? For

More information

MODULE 4: ABSORPTION

MODULE 4: ABSORPTION MODULE 4: ABSORPTION LECTURE NO. 3 4.4. Deign of packed tower baed on overall ma tranfer coefficient * From overall ma tranfer equation, N K ( y y ) one can write for packed tower a N A K y (y-y*) Then,

More information

Solutions. Digital Control Systems ( ) 120 minutes examination time + 15 minutes reading time at the beginning of the exam

Solutions. Digital Control Systems ( ) 120 minutes examination time + 15 minutes reading time at the beginning of the exam BSc - Sample Examination Digital Control Sytem (5-588-) Prof. L. Guzzella Solution Exam Duration: Number of Quetion: Rating: Permitted aid: minute examination time + 5 minute reading time at the beginning

More information

USPAS Course on Recirculated and Energy Recovered Linear Accelerators

USPAS Course on Recirculated and Energy Recovered Linear Accelerators USPAS Coure on Recirculated and Energy Recovered Linear Accelerator G. A. Krafft and L. Merminga Jefferon Lab I. Bazarov Cornell Lecture 6 7 March 005 Lecture Outline. Invariant Ellipe Generated by a Unimodular

More information

Theoretical study of the dual harmonic system and its application on the CSNS/RCS

Theoretical study of the dual harmonic system and its application on the CSNS/RCS Theoretical tudy of the dual harmonic ytem and it application on the CSNS/RCS Yao-Shuo Yuan, Na Wang, Shou-Yan Xu, Yue Yuan, and Sheng Wang Dongguan branch, Intitute of High Energy Phyic, CAS, Guangdong

More information

PI control system design for Electromagnetic Molding Machine based on Linear Programing

PI control system design for Electromagnetic Molding Machine based on Linear Programing PI control ytem deign for Electromagnetic Molding Machine baed on Linear Programing Takayuki Ihizaki, Kenji Kahima, Jun-ichi Imura*, Atuhi Katoh and Hirohi Morita** Abtract In thi paper, we deign a PI

More information

BASIC INDUCTION MOTOR CONCEPTS

BASIC INDUCTION MOTOR CONCEPTS INDUCTION MOTOS An induction motor ha the ame phyical tator a a ynchronou machine, with a different rotor contruction. There are two different type of induction motor rotor which can be placed inide the

More information

Behavioral Modeling of Transmission Line Channels via Linear Transformations

Behavioral Modeling of Transmission Line Channels via Linear Transformations Behavioral Modeling of Tranmiion Line Channel via Linear Tranformation Albert Vareljian albertv@ieeeorg Member, IEEE, Canada Abtract An approach baed on the linear tranformation of network port variable

More information

EECS 242: Amplifier Design Examples

EECS 242: Amplifier Design Examples EECS 242: Amplifier Design Examples Small-Signal Transistor Model Intrinsic transistor model Using basic equations, let s assume we have the following process: f T = 100 GHz A v0 = 10, V t = 0.3V, V gs

More information

Earth Potential Rise (EPR) Computation for a Fault on Transmission Mains Pole

Earth Potential Rise (EPR) Computation for a Fault on Transmission Mains Pole ACN: 32586675 ABN: 8632586675 NATIONAL ELECTRICAL ENGINEERING CONULTANCY Earth otential Rie (ER) Computation for a Fault on Tranmiion Main ole repared by: M. Naereddine ACN: 32586675 ABN: 8632586675 Abtract

More information

9 Lorentz Invariant phase-space

9 Lorentz Invariant phase-space 9 Lorentz Invariant phae-space 9. Cro-ection The cattering amplitude M q,q 2,out p, p 2,in i the amplitude for a tate p, p 2 to make a tranition into the tate q,q 2. The tranition probability i the quare

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

f max = GHz I ave PartAData 2 :=

f max = GHz I ave PartAData 2 := NTU 6342 / EE 24 Homework #3 SOLUTIONS Problem #: Delay time: t p_fo4_2 :=.424n t p_fo4_ := 2.2n Simulation value: T min := 2 t p_fo4_2 T max := 2 t p_fo4_ T min =.848 n T max = 4.24 n f max := T min Part

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

Correction for Simple System Example and Notes on Laplace Transforms / Deviation Variables ECHE 550 Fall 2002

Correction for Simple System Example and Notes on Laplace Transforms / Deviation Variables ECHE 550 Fall 2002 Correction for Simple Sytem Example and Note on Laplace Tranform / Deviation Variable ECHE 55 Fall 22 Conider a tank draining from an initial height of h o at time t =. With no flow into the tank (F in

More information

Neural Network Linearization of Pressure Force Sensor Transfer Characteristic

Neural Network Linearization of Pressure Force Sensor Transfer Characteristic Acta Polytechnica Hungarica Vol., No., 006 Neural Network Linearization of Preure Force Senor Tranfer Characteritic Jozef Vojtko, Irena Kováčová, Ladilav Madaráz, Dobrolav Kováč Faculty of Electrical Engineering

More information

Homework 12 Solution - AME30315, Spring 2013

Homework 12 Solution - AME30315, Spring 2013 Homework 2 Solution - AME335, Spring 23 Problem :[2 pt] The Aerotech AGS 5 i a linear motor driven XY poitioning ytem (ee attached product heet). A friend of mine, through careful experimentation, identified

More information

Lecture 12 Date:

Lecture 12 Date: Lecture 12 Date: 09.02.2017 Microstrip Matching Networks Series- and Shunt-stub Matching Quarter Wave Impedance Transformer Microstrip Line Matching Networks In the lower RF region, its often a standard

More information

R. W. Erickson. Department of Electrical, Computer, and Energy Engineering University of Colorado, Boulder

R. W. Erickson. Department of Electrical, Computer, and Energy Engineering University of Colorado, Boulder R. W. Erickon Department of Electrical, Computer, and Energy Engineering Univerity of Colorado, Boulder ZOH: Sampled Data Sytem Example v T Sampler v* H Zero-order hold H v o e = 1 T 1 v *( ) = v( jkω

More information

Homework #7 Solution. Solutions: ΔP L Δω. Fig. 1

Homework #7 Solution. Solutions: ΔP L Δω. Fig. 1 Homework #7 Solution Aignment:. through.6 Bergen & Vittal. M Solution: Modified Equation.6 becaue gen. peed not fed back * M (.0rad / MW ec)(00mw) rad /ec peed ( ) (60) 9.55r. p. m. 3600 ( 9.55) 3590.45r.

More information

ECEN620: Network Theory Broadband Circuit Design Fall 2018

ECEN620: Network Theory Broadband Circuit Design Fall 2018 ECEN60: Network Theory Broadband Circuit Deign Fall 08 Lecture 6: Loop Filter Circuit Sam Palermo Analog & Mixed-Signal Center Texa A&M Univerity Announcement HW i due Oct Require tranitor-level deign

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

JCP Software & Company, Inc

JCP Software & Company, Inc lide-rule TM for Microsoft Windows Microwave Transistor Amplifier Design Introduction and Reference Manual unstable. unstable L. VWR(out) db NF OPT L.4 db..8 db.6 db.. Ga 8 db Ga 7 db Ga 6 db. JCP oftware

More information

Liquid cooling

Liquid cooling SKiiPPACK no. 3 4 [ 1- exp (-t/ τ )] + [( P + P )/P ] R [ 1- exp (-t/ τ )] Z tha tot3 = R ν ν tot1 tot tot3 thaa-3 aa 3 ν= 1 3.3.6. Liquid cooling The following table contain the characteritic R ν and

More information

A new approach to determinate parasitic elements of GaN HEMT by COLD FET S-Parameter

A new approach to determinate parasitic elements of GaN HEMT by COLD FET S-Parameter A ne approach to determinate paraitic element of GaN HEMT by COLD FET -Parameter Min Han 1*, Yongheng Dai 1, 2, Jianjun Zhou 2, Chao Liu 3, Xu Li 1 1 chool of Electronic and Optical Engineer,Nanjing Univerity

More information

MODERN CONTROL SYSTEMS

MODERN CONTROL SYSTEMS MODERN CONTROL SYSTEMS Lecture 1 Root Locu Emam Fathy Department of Electrical and Control Engineering email: emfmz@aat.edu http://www.aat.edu/cv.php?dip_unit=346&er=68525 1 Introduction What i root locu?

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

Massachusetts Institute of Technology Dynamics and Control II

Massachusetts Institute of Technology Dynamics and Control II I E Maachuett Intitute of Technology Department of Mechanical Engineering 2.004 Dynamic and Control II Laboratory Seion 5: Elimination of Steady-State Error Uing Integral Control Action 1 Laboratory Objective:

More information

Lecture 23 Date:

Lecture 23 Date: Lecture 3 Date: 4.4.16 Plane Wave in Free Space and Good Conductor Power and Poynting Vector Wave Propagation in Loy Dielectric Wave propagating in z-direction and having only x-component i given by: E

More information

Lecture 17: Analytic Functions and Integrals (See Chapter 14 in Boas)

Lecture 17: Analytic Functions and Integrals (See Chapter 14 in Boas) Lecture 7: Analytic Function and Integral (See Chapter 4 in Boa) Thi i a good point to take a brief detour and expand on our previou dicuion of complex variable and complex function of complex variable.

More information

ABSTRACT- In this paper, a Shunt active power filter (SAPF) is developed without considering any harmonic detection

ABSTRACT- In this paper, a Shunt active power filter (SAPF) is developed without considering any harmonic detection Special Iue of International Journal of Advance in Applied Science and Engineering (IJAEAS) ISSN (P): 2348-1811; ISSN (E): 2348-182X Vol. 4, Iue 1,2, March 2017, 34-39 IIST SHUNT ACTIVE POWER FILTER PERFORMANCE

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

Entropy Minimization in Design of Extractive Distillation System with Internal Heat Exchangers

Entropy Minimization in Design of Extractive Distillation System with Internal Heat Exchangers Entropy Minimization in Deign of Extractive Ditillation Sytem with Internal Heat Exchanger Diego F. Mendoza, Carlo.M. Riaco * Group of Proce Sytem Engineering, Department of Chemical and Environmental

More information

A Simplified Methodology for the Synthesis of Adaptive Flight Control Systems

A Simplified Methodology for the Synthesis of Adaptive Flight Control Systems A Simplified Methodology for the Synthei of Adaptive Flight Control Sytem J.ROUSHANIAN, F.NADJAFI Department of Mechanical Engineering KNT Univerity of Technology 3Mirdamad St. Tehran IRAN Abtract- A implified

More information

1 Routh Array: 15 points

1 Routh Array: 15 points EE C28 / ME34 Problem Set 3 Solution Fall 2 Routh Array: 5 point Conider the ytem below, with D() k(+), w(t), G() +2, and H y() 2 ++2 2(+). Find the cloed loop tranfer function Y () R(), and range of k

More information

MAXIMUM BENDING MOMENT AND DUCTILITY OF R/HPFRCC BEAMS

MAXIMUM BENDING MOMENT AND DUCTILITY OF R/HPFRCC BEAMS MAXIMUM BENDING MOMENT AND DUCTILITY OF R/HPFRCC BEAMS Aleandro P. Fantilli 1, Hirozo Mihahi 2 and Paolo Vallini 1 (1) Politecnico di Torino, Torino, Italy (2) Tohoku Univerity, Sendai, Japan Abtract The

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

MAHALAKSHMI ENGINEERING COLLEGE-TRICHY

MAHALAKSHMI ENGINEERING COLLEGE-TRICHY DIGITAL SIGNAL PROCESSING DEPT./SEM.: CSE /VII DIGITAL FILTER DESIGN-IIR & FIR FILTER DESIGN PART-A. Lit the different type of tructure for realiation of IIR ytem? AUC APR 09 The different type of tructure

More information

Annexure-I. network acts as a buffer in matching the impedance of the plasma reactor to that of the RF

Annexure-I. network acts as a buffer in matching the impedance of the plasma reactor to that of the RF Annexure-I Impedance matching and Smith chart The output impedance of the RF generator is 50 ohms. The impedance matching network acts as a buffer in matching the impedance of the plasma reactor to that

More information

Study on the effect of vent on the electroacoustic absorber

Study on the effect of vent on the electroacoustic absorber INTER-NOISE 016 Study on the effect of vent on the electroacoutic aborber Youngeun Cho 1 ; Semyung Wang 1, Gwangju Intitute of Science and Technology, Republic of Korea ABSTRACT Electroacoutic aborber

More information

Experimental Verification of Optimal Sliding Mode Controllers for Hoisting Cranes

Experimental Verification of Optimal Sliding Mode Controllers for Hoisting Cranes Experimental Verification of Optimal Sliding Mode Controller for Hoiting Crane Alekandra Nowacka-Leverton Dariuz Pazderki Maciej Micha lek Andrzej Bartozewicz Intitute of Automatic Control, Technical Univerity

More information

Analysis of Step Response, Impulse and Ramp Response in the Continuous Stirred Tank Reactor System

Analysis of Step Response, Impulse and Ramp Response in the Continuous Stirred Tank Reactor System ISSN: 454-50 Volume 0 - Iue 05 May 07 PP. 7-78 Analyi of Step Repone, Impule and Ramp Repone in the ontinuou Stirred Tank Reactor Sytem * Zohreh Khohraftar, Pirouz Derakhhi, (Department of hemitry, Science

More information

Control Systems Engineering ( Chapter 7. Steady-State Errors ) Prof. Kwang-Chun Ho Tel: Fax:

Control Systems Engineering ( Chapter 7. Steady-State Errors ) Prof. Kwang-Chun Ho Tel: Fax: Control Sytem Engineering ( Chapter 7. Steady-State Error Prof. Kwang-Chun Ho kwangho@hanung.ac.kr Tel: 0-760-453 Fax:0-760-4435 Introduction In thi leon, you will learn the following : How to find the

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

Convergence criteria and optimization techniques for beam moments

Convergence criteria and optimization techniques for beam moments Pure Appl. Opt. 7 (1998) 1221 1230. Printed in the UK PII: S0963-9659(98)90684-5 Convergence criteria and optimization technique for beam moment G Gbur and P S Carney Department of Phyic and Atronomy and

More information

Simple Observer Based Synchronization of Lorenz System with Parametric Uncertainty

Simple Observer Based Synchronization of Lorenz System with Parametric Uncertainty IOSR Journal of Electrical and Electronic Engineering (IOSR-JEEE) ISSN: 78-676Volume, Iue 6 (Nov. - Dec. 0), PP 4-0 Simple Oberver Baed Synchronization of Lorenz Sytem with Parametric Uncertainty Manih

More information