SAMPLING. Sampling is the acquisition of a continuous signal at discrete time intervals and is a fundamental concept in real-time signal processing.

Size: px
Start display at page:

Download "SAMPLING. Sampling is the acquisition of a continuous signal at discrete time intervals and is a fundamental concept in real-time signal processing."

Transcription

1 SAMPLING Sampling i the acquiition of a continuou ignal at dicrete time interval and i a fundamental concept in real-time ignal proceing. he actual ampling operation can alo be defined by the figure belo and a can be een i a MODULAION proce. he carrier ignal δ (t) i a train of impule. x(t) x (t) δ () t = δ ( t n ) n= he output of the modulator i x (t) and i given by: x () t = x() t δ () t = x() t δ ( t n ) n= If e recall that convolution by a hifted impule i the ignal hifted by the ame amount then () t = x( n ) ( t n ) n= x δ hi relation decribe the ampling proce in the time-domain. he ampling frequency F =.0/ mut be elected large enough uch that the ampling proce ill not reult in any lo of pectral information (no-aliaing). We ill invetigate the ampling operation further by taking the Fourier ranform of x () t. he Fourier ranform of the impule train: F { δ () t } = F δ ( t n ) = δ ( n ) n= π n=

2 π here = = πf here f i the ampling frequency in Hz. Alo e recall that multiplication in time i convolution in frequency domain. X π ( ) = X ( ) F{ δ ( t) } = X ( ) δ ( n ) π π n= but e already kno that X ( ) δ ( ) = X ( ) X ( ) = X ( ) n n= () Firt let x(t) be band limited in frequency uch that X() = 0 for > M. hi e can ho a in the diagram belo: X() - M M Next aume that the highet frequency in X() i le than one-half the ampling frequency: M < From equation () e note that the effect of the impule ampling of x(t) i to replicate the frequency pectrum of X() about the frequencie n = ±, ±, ± 3,.a hon belo:

3 X () / Fig. 3. For thi cae e can recover the ignal x(t) exactly from it ample x[n] uing an ideal lo-pa filter. We call the recovery of a ignal from it ample DAA RECONSRUCION. No aume the cae hen the highet frequency in x(t) i greater than /. he ne plot ill be a hon belo; / Fig. 3. For the cae in Fig. 3. x(t) can be recovered exactly from x (t) by mean of a lopa filter ith gain and a cutoff frequency greater than M and le than ( M ). Belo i the block diagram hoing the ue of the lopa filter:

4 δ () t x(t) x (t) h(t) H(j) x r (t) If e aume that the pectrum of x(t) i a hon belo X() - M M and aume that the ampling frequency > M then the pectrum of the ampled ignal ill be a hon belo: X (j) / M 0 M No if e elect the cutoff frequency of the lopa filter to be beteen M and ( M ) the characteritic curve for the filter ill be a hon belo:

5 H(j) - c c he pectrum of the recontructed ignal x r (t) ill then be a follo: X r (j) - M M Note that in Fig. 3. frequency component overlap in the ampled ignal and x(t) can not be recovered by lopa filtering. A requirement for ampling i the folloing: Sampling frequency mut be at leat tice a great a the highet frequency M in the ignal that i ampled.

6 No let u conider practical ampling. A phyical ignal cannot be bandlimited in frequency. Hoever a phyical ignal doe exit uch that the amplitude of the frequency pectrum above a certain frequency i o mall that it i negligible. We ee that an other requirement for ampling i that: Frequency pectrum of the ignal be inignificant above the frequency here = πf and f i the ampling frequency. f Frequency i called the NYQUIS frequency. hi i alo knon a Shannon Sampling heorem. Sampling With a Zero Order Hold. Sampling theorem a explained in term of impule-train ampling. Hoever in practice, narro large-amplitude pule hich approximate impule are relatively difficult to generate and tranmit. It i often more convenient to generate the ampled ignal in a form knon a a zeroorder hold. hi ytem ample x(t) at a given time intant and hold that value until the next intant.

7 x(t) Zero Order Hold x o (t) he recontruction of x(t) from the output of a zero-order hold can be achieved by lopa filtering. Hoever the required filter no longer ha contant gain in the paband. Let u try to develop thi filter characteritic curve. We note that x o (t) can be generated by impule train ampling folloed by an LI ytem ith a rectangular impule repone a hon belo: p () t x(t) x p (t) h 0 (t) x o (t) 0 x(t) x p (t) x o (t) o recontruct x(t) from x o (t) e conider proceing x o (t) ith an LI ytem ith impule repone x r (t).

8 p () t H(j) x(t) x p (t) h 0 (t) 0 x o (t) h r (t) H r (j) r(t) We need to pecify H r (j) o that r(t) = x(t). We note that thi ill only be true if the cacade combination of h 0 (t) and h r (t) i the ideal lopa filter H(j). Or imilarly H(j) = H 0 (j).h r (j) But e kno that the pectrum of h 0 (t) i: H 0 j = in / ( j) e hence it i required that H r ( j) j e H ( j) = () in( / ) for example ith cutoff frequency of / the ideal magnitude and phae for the recontruction filter folloing a zero-order hold i a belo:

9 H r (j) π/ H r (j) -π/ We note that the actual realization of equation () i not poible ithout an approximation. In fact in many ituation the output of the zero-order hold i conidered an adequate approximation to the original ignal by itelf. Alternatively in ome application e may ih to perform a moother interpolation beteen ample value. o important form of data recontruction exit:. Interpolation (uitable for data tranmiion ytem). extrapolation (uitable for feedback ytem) Extrapolation i interpolation extended to point outide the convex hull of a dataet. Interpolation value at a point outide the convex hull of an input dataet i referred to a an extrapolated value.

10 Interpolation I the fitting of a continuou ignal to a et of ample value. One imple interpolation procedure i the zero order hold previouly dicued. An other ueful form of interpolation i linear interpolation here adjacent point are connected by a traight line a een belo: We have een before that if the ampling intant are ufficiently cloe, then the ignal i recontructed exactly. i.e. through the ue of a lopa filter exact interpolation can be carried out beteen the ample point. Conider in the time-domain the effect of the lopa filter x ( t) = x r or x ( t) = r p n= ( t) h( t) x( n ) h( t n ) For the ideal lopa filter H(j), h(t) i a follo c in( ct) h( t) = π t c

11 Interpolation Uing Matlab YI = INERP( X,Y,XI) hi matlab command ill find YI uing value of the underlying function Y. It carrie out interpolation for the point in vector XI. Vector X pecifie the point at hich the data Y i given Interpolation i the ame operation a table lookup. Decribed in table look up term INERP look up the element of XI in X and baed upon their location return value YI interpolated ithin the element of Y. Uage: YI = INERP(X,Y,XI, method ); nearet : nearet neighbor interpolation linear : linear interpolation pline : cubic pline interpolation cubic : cubic interpolation Example: x = 0:0; y= in(x); xi = 0:0.5:0; yi = interp(x,y,xi); plot(x,y, o,xi,yi, * ) x = >> y y = Column through Column

12 >> xi xi = Column through Column through Column through Column 3 through Column >> yi yi = Column through Column through Column through Column 3 through Column >>

13

EE 477 Digital Signal Processing. 4 Sampling; Discrete-Time

EE 477 Digital Signal Processing. 4 Sampling; Discrete-Time EE 477 Digital Signal Proceing 4 Sampling; Dicrete-Time Sampling a Continuou Signal Obtain a equence of ignal ample uing a periodic intantaneou ampler: x [ n] = x( nt ) Often plot dicrete ignal a dot or

More information

Sampling and the Discrete Fourier Transform

Sampling and the Discrete Fourier Transform Sampling and the Dicrete Fourier Tranform Sampling Method Sampling i mot commonly done with two device, the ample-and-hold (S/H) and the analog-to-digital-converter (ADC) The S/H acquire a CT ignal at

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

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 4: Applications of Fourier Representations. Chih-Wei Liu

Chapter 4: Applications of Fourier Representations. Chih-Wei Liu Chapter 4: Application of Fourier Repreentation Chih-Wei Liu Outline Introduction Fourier ranform of Periodic Signal Convolution/Multiplication with Non-Periodic Signal Fourier ranform of Dicrete-ime Signal

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

Chapter 2: Problem Solutions

Chapter 2: Problem Solutions Chapter 2: Solution Dicrete Time Proceing of Continuou Time Signal Sampling à 2.. : Conider a inuoidal ignal and let u ample it at a frequency F 2kHz. xt 3co000t 0. a) Determine and expreion for the ampled

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

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

Spring 2014 EE 445S Real-Time Digital Signal Processing Laboratory. Homework #0 Solutions on Review of Signals and Systems Material

Spring 2014 EE 445S Real-Time Digital Signal Processing Laboratory. Homework #0 Solutions on Review of Signals and Systems Material Spring 4 EE 445S Real-Time Digital Signal Proceing Laboratory Prof. Evan Homework # Solution on Review of Signal and Sytem Material Problem.. Continuou-Time Sinuoidal Generation. In practice, we cannot

More information

5.5 Sampling. The Connection Between: Continuous Time & Discrete Time

5.5 Sampling. The Connection Between: Continuous Time & Discrete Time 5.5 Sampling he Connection Between: Continuou ime & Dicrete ime Warning: I don t really like how the book cover thi! It i not that it i wrong it jut ail to make the correct connection between the mathematic

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

Digital Control System

Digital Control System Digital Control Sytem Summary # he -tranform play an important role in digital control and dicrete ignal proceing. he -tranform i defined a F () f(k) k () A. Example Conider the following equence: f(k)

More information

Roadmap for Discrete-Time Signal Processing

Roadmap for Discrete-Time Signal Processing EE 4G Note: Chapter 8 Continuou-time Signal co(πf Roadmap for Dicrete-ime Signal Proceing.5 -.5 -..4.6.8..4.6.8 Dicrete-time Signal (Section 8.).5 -.5 -..4.6.8..4.6.8 Sampling Period econd (or ampling

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

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

1 Bertrand duopoly with incomplete information

1 Bertrand duopoly with incomplete information Game Theory Solution to Problem Set 5 1 Bertrand duopoly ith incomplete information The game i de ned by I = f1; g ; et of player A i = [0; 1) T i = fb L ; b H g, ith p(b L ) = u i (b i ; p i ; p j ) =

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

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

FRTN10 Exercise 3. Specifications and Disturbance Models

FRTN10 Exercise 3. Specifications and Disturbance Models FRTN0 Exercie 3. Specification and Diturbance Model 3. A feedback ytem i hown in Figure 3., in which a firt-order proce if controlled by an I controller. d v r u 2 z C() P() y n Figure 3. Sytem in Problem

More information

Determination of the local contrast of interference fringe patterns using continuous wavelet transform

Determination of the local contrast of interference fringe patterns using continuous wavelet transform Determination of the local contrat of interference fringe pattern uing continuou wavelet tranform Jong Kwang Hyok, Kim Chol Su Intitute of Optic, Department of Phyic, Kim Il Sung Univerity, Pyongyang,

More information

Lecture 5 Frequency Response of FIR Systems (III)

Lecture 5 Frequency Response of FIR Systems (III) EE3054 Signal and Sytem Lecture 5 Frequency Repone of FIR Sytem (III Yao Wang Polytechnic Univerity Mot of the lide included are extracted from lecture preentation prepared by McClellan and Schafer Licene

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

DYNAMIC MODELS FOR CONTROLLER DESIGN

DYNAMIC MODELS FOR CONTROLLER DESIGN DYNAMIC MODELS FOR CONTROLLER DESIGN M.T. Tham (996,999) Dept. of Chemical and Proce Engineering Newcatle upon Tyne, NE 7RU, UK.. INTRODUCTION The problem of deigning a good control ytem i baically that

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

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

The Laplace Transform

The Laplace Transform The Laplace Tranform Prof. Siripong Potiuk Pierre Simon De Laplace 749-827 French Atronomer and Mathematician Laplace Tranform An extenion of the CT Fourier tranform to allow analyi of broader cla of CT

More information

Filter Dispersion. with respect to frequency otherwise signal dispersion (and thus signal distortion) will result. Right?

Filter Dispersion. with respect to frequency otherwise signal dispersion (and thus signal distortion) will result. Right? 3/1/005 Filter Diperion.doc 1/6 Filter Diperion Any ignal that carrie ignificant information mut ha ome non-zero bandwidth. In other word, the ignal energy (a well a the information it carrie) i pread

More information

RaneNote BESSEL FILTER CROSSOVER

RaneNote BESSEL FILTER CROSSOVER RaneNote BESSEL FILTER CROSSOVER A Beel Filter Croover, and It Relation to Other Croover Beel Function Phae Shift Group Delay Beel, 3dB Down Introduction One of the way that a croover may be contructed

More information

Stability Criterion Routh Hurwitz

Stability Criterion Routh Hurwitz EES404 Fundamental of Control Sytem Stability Criterion Routh Hurwitz DR. Ir. Wahidin Wahab M.Sc. Ir. Arie Subiantoro M.Sc. Stability A ytem i table if for a finite input the output i imilarly finite A

More information

( ) ( ) ω = X x t e dt

( ) ( ) ω = X x t e dt The Laplace Tranform The Laplace Tranform generalize the Fourier Traform for the entire complex plane For an ignal x(t) the pectrum, or it Fourier tranform i (if it exit): t X x t e dt ω = For the ame

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

GNSS Solutions: What is the carrier phase measurement? How is it generated in GNSS receivers? Simply put, the carrier phase

GNSS Solutions: What is the carrier phase measurement? How is it generated in GNSS receivers? Simply put, the carrier phase GNSS Solution: Carrier phae and it meaurement for GNSS GNSS Solution i a regular column featuring quetion and anwer about technical apect of GNSS. Reader are invited to end their quetion to the columnit,

More information

LRA DSP. Multi-Rate DSP. Applications: Oversampling, Undersampling, Quadrature Mirror Filters. Professor L R Arnaut 1

LRA DSP. Multi-Rate DSP. Applications: Oversampling, Undersampling, Quadrature Mirror Filters. Professor L R Arnaut 1 ulti-rate Application: Overampling, Underampling, Quadrature irror Filter Profeor L R Arnaut ulti-rate Overampling Profeor L R Arnaut Optimal Sampling v. Overampling Sampling at Nyquit rate F =F B Allow

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

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

Properties of Z-transform Transform 1 Linearity a

Properties of Z-transform Transform 1 Linearity a Midterm 3 (Fall 6 of EEG:. Thi midterm conit of eight ingle-ided page. The firt three page contain variou table followed by FOUR eam quetion and one etra workheet. You can tear out any page but make ure

More information

LTV System Modelling

LTV System Modelling Helinki Univerit of Technolog S-72.333 Potgraduate Coure in Radiocommunication Fall 2000 LTV Stem Modelling Heikki Lorentz Sonera Entrum O heikki.lorentz@onera.fi Januar 23 rd 200 Content. Introduction

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

Mathematical modeling of control systems. Laith Batarseh. Mathematical modeling of control systems

Mathematical modeling of control systems. Laith Batarseh. Mathematical modeling of control systems Chapter two Laith Batareh Mathematical modeling The dynamic of many ytem, whether they are mechanical, electrical, thermal, economic, biological, and o on, may be decribed in term of differential equation

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

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

Digital Transmission of Analog Signals: PCM, DPCM and DM

Digital Transmission of Analog Signals: PCM, DPCM and DM A T CHAPTER 6 Digital Tranmiion of Analog Signal: PCM, DPCM and DM 6.1 Introduction Quite a few of the information bearing ignal, uch a peech, muic, video, etc., are analog in nature; that i, they are

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

Lecture 2: The z-transform

Lecture 2: The z-transform 5-59- Control Sytem II FS 28 Lecture 2: The -Tranform From the Laplace Tranform to the tranform The Laplace tranform i an integral tranform which take a function of a real variable t to a function of a

More information

Convex Hulls of Curves Sam Burton

Convex Hulls of Curves Sam Burton Convex Hull of Curve Sam Burton 1 Introduction Thi paper will primarily be concerned with determining the face of convex hull of curve of the form C = {(t, t a, t b ) t [ 1, 1]}, a < b N in R 3. We hall

More information

CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS

CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.1 INTRODUCTION 8.2 REDUCED ORDER MODEL DESIGN FOR LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.3

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

EELE 3332 Electromagnetic II Chapter 10

EELE 3332 Electromagnetic II Chapter 10 EELE 333 Electromagnetic II Chapter 10 Electromagnetic Wave Propagation Ilamic Univerity of Gaza Electrical Engineering Department Dr. Talal Skaik 01 1 Electromagnetic wave propagation A changing magnetic

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

S_LOOP: SINGLE-LOOP FEEDBACK CONTROL SYSTEM ANALYSIS

S_LOOP: SINGLE-LOOP FEEDBACK CONTROL SYSTEM ANALYSIS S_LOOP: SINGLE-LOOP FEEDBACK CONTROL SYSTEM ANALYSIS by Michelle Gretzinger, Daniel Zyngier and Thoma Marlin INTRODUCTION One of the challenge to the engineer learning proce control i relating theoretical

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

Data Converters. Introduction. Overview. The ideal data converter. Sampling. x t x nt x t t nt

Data Converters. Introduction. Overview. The ideal data converter. Sampling. x t x nt x t t nt Data Converter Overview Introduction Pietro Andreani Dept. of Electrical and Information echnology Lund Univerity, Sweden Introduction he ideal A/D and D/A data converter Sampling Amplitude quantization

More information

SIMPLIFIED MODEL FOR EPICYCLIC GEAR INERTIAL CHARACTERISTICS

SIMPLIFIED MODEL FOR EPICYCLIC GEAR INERTIAL CHARACTERISTICS UNIVERSITY OF PITESTI SCIENTIFIC BULLETIN FACULTY OF ECHANICS AND TECHNOLOGY AUTOOTIVE erie, year XVII, no. ( 3 ) SIPLIFIED ODEL FOR EPICYCLIC GEAR INERTIAL CHARACTERISTICS Ciobotaru, Ticuşor *, Feraru,

More information

Real Sources (Secondary Sources) Phantom Source (Primary source) LS P. h rl. h rr. h ll. h lr. h pl. h pr

Real Sources (Secondary Sources) Phantom Source (Primary source) LS P. h rl. h rr. h ll. h lr. h pl. h pr Ecient frequency domain ltered-x realization of phantom ource iet C.W. ommen, Ronald M. Aart, Alexander W.M. Mathijen, John Gara, Haiyan He Abtract A phantom ound ource i a virtual ound image which can

More information

Advanced Digital Signal Processing. Stationary/nonstationary signals. Time-Frequency Analysis... Some nonstationary signals. Time-Frequency Analysis

Advanced Digital Signal Processing. Stationary/nonstationary signals. Time-Frequency Analysis... Some nonstationary signals. Time-Frequency Analysis Advanced Digital ignal Proceing Prof. Nizamettin AYDIN naydin@yildiz.edu.tr Time-Frequency Analyi http://www.yildiz.edu.tr/~naydin 2 tationary/nontationary ignal Time-Frequency Analyi Fourier Tranform

More information

Efficient Methods of Doppler Processing for Coexisting Land and Weather Clutter

Efficient Methods of Doppler Processing for Coexisting Land and Weather Clutter Efficient Method of Doppler Proceing for Coexiting Land and Weather Clutter Ça gatay Candan and A Özgür Yılmaz Middle Eat Technical Univerity METU) Ankara, Turkey ccandan@metuedutr, aoyilmaz@metuedutr

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

SMALL-SIGNAL STABILITY ASSESSMENT OF THE EUROPEAN POWER SYSTEM BASED ON ADVANCED NEURAL NETWORK METHOD

SMALL-SIGNAL STABILITY ASSESSMENT OF THE EUROPEAN POWER SYSTEM BASED ON ADVANCED NEURAL NETWORK METHOD SMALL-SIGNAL STABILITY ASSESSMENT OF THE EUROPEAN POWER SYSTEM BASED ON ADVANCED NEURAL NETWORK METHOD S.P. Teeuwen, I. Erlich U. Bachmann Univerity of Duiburg, Germany Department of Electrical Power Sytem

More information

Fading Channels: Capacity, BER and Diversity

Fading Channels: Capacity, BER and Diversity Fading Channel: Capacity, BER and Diverity Mater Univeritario en Ingeniería de Telecomunicación I. Santamaría Univeridad de Cantabria Introduction Capacity BER Diverity Concluion Content Introduction Capacity

More information

Main Topics: The Past, H(s): Poles, zeros, s-plane, and stability; Decomposition of the complete response.

Main Topics: The Past, H(s): Poles, zeros, s-plane, and stability; Decomposition of the complete response. EE202 HOMEWORK PROBLEMS SPRING 18 TO THE STUDENT: ALWAYS CHECK THE ERRATA on the web. Quote for your Parent' Partie: 1. Only with nodal analyi i the ret of the emeter a poibility. Ray DeCarlo 2. (The need

More information

1 Basic Equations of the PLLs

1 Basic Equations of the PLLs 1 Baic Equation of the PLL 1.1 INTRODUCTION Phae lock loop (PLL) belong to a larger et of regulation ytem. A an independent reearch and deign field it tarted in the 1950 [1] and gained major practical

More information

SINGLE CARRIER BLOCK TRANSMISSION WITHOUT GUARD INTERVAL

SINGLE CARRIER BLOCK TRANSMISSION WITHOUT GUARD INTERVAL SINGLE CARRIER BLOCK TRANSMISSION WITHOUT GUARD INTERVAL Kazunori Hayahi Hideaki Sakai Graduate School of Informatic, Kyoto Univerity Kyoto, JAPAN ABSTRACT Thi paper propoe a imple detection cheme for

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 5 Optimum Receivers for the Additive White Gaussian Noise Channel

Chapter 5 Optimum Receivers for the Additive White Gaussian Noise Channel Chapter 5 Optimum Receiver for the Additive White Gauian Noie Channel Table of Content 5.1 Optimum Receiver for Signal Corrupted by Additive White Noie 5.1.1 Correlation Demodulator 5.1. Matched-Filter

More information

Finite Element Analysis of a Fiber Bragg Grating Accelerometer for Performance Optimization

Finite Element Analysis of a Fiber Bragg Grating Accelerometer for Performance Optimization Finite Element Analyi of a Fiber Bragg Grating Accelerometer for Performance Optimization N. Baumallick*, P. Biwa, K. Dagupta and S. Bandyopadhyay Fiber Optic Laboratory, Central Gla and Ceramic Reearch

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

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

Hybrid Projective Dislocated Synchronization of Liu Chaotic System Based on Parameters Identification

Hybrid Projective Dislocated Synchronization of Liu Chaotic System Based on Parameters Identification www.ccenet.org/ma Modern Applied Science Vol. 6, No. ; February Hybrid Projective Dilocated Synchronization of Liu Chaotic Sytem Baed on Parameter Identification Yanfei Chen College of Science, Guilin

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

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

March 18, 2014 Academic Year 2013/14

March 18, 2014 Academic Year 2013/14 POLITONG - SHANGHAI BASIC AUTOMATIC CONTROL Exam grade March 8, 4 Academic Year 3/4 NAME (Pinyin/Italian)... STUDENT ID Ue only thee page (including the back) for anwer. Do not ue additional heet. Ue of

More information

EE Control Systems LECTURE 14

EE Control Systems LECTURE 14 Updated: Tueday, March 3, 999 EE 434 - Control Sytem LECTURE 4 Copyright FL Lewi 999 All right reerved ROOT LOCUS DESIGN TECHNIQUE Suppoe the cloed-loop tranfer function depend on a deign parameter k We

More information

Exercises for lectures 19 Polynomial methods

Exercises for lectures 19 Polynomial methods Exercie for lecture 19 Polynomial method Michael Šebek Automatic control 016 15-4-17 Diviion of polynomial with and without remainder Polynomial form a circle, but not a body. (Circle alo form integer,

More information

An Efficient Class of Estimators for the Finite Population Mean in Ranked Set Sampling

An Efficient Class of Estimators for the Finite Population Mean in Ranked Set Sampling Open Journal of Statitic 06 6 46-435 Publihed Online June 06 in SciRe http://cirporg/journal/oj http://ddoiorg/0436/oj0663038 An Efficient Cla of Etimator for the Finite Population Mean in Ranked Set Sampling

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

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

Convex Optimization-Based Rotation Parameter Estimation Using Micro-Doppler

Convex Optimization-Based Rotation Parameter Estimation Using Micro-Doppler Journal of Electrical Engineering 4 (6) 57-64 doi:.765/8-/6.4. D DAVID PUBLISHING Convex Optimization-Baed Rotation Parameter Etimation Uing Micro-Doppler Kyungwoo Yoo, Joohwan Chun, Seungoh Yoo and Chungho

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

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

DETECTION OF ROOM REFLECTIONS FROM A BINAURAL ROOM IMPULSE RESPONSE

DETECTION OF ROOM REFLECTIONS FROM A BINAURAL ROOM IMPULSE RESPONSE Sampo Vea and Tapio Lokki. 2006. Detection of room reflection from a binaural room impule repone. In: Proceeding of the 9th International Conference on Digital Audio Effect (DAFx 2006). Montreal, Canada.

More information

Demonstration of inverse scattering in optical coherence tomography

Demonstration of inverse scattering in optical coherence tomography Demontration of invere cattering in optical coherence tomography Tyler S. Ralton a,b, Dan Mark a,b, P. Scott Carney a,b, and Stephen A. Boppart a,b,c,* a Beckman ntitute for Advanced Science and Technology

More information

Wolfgang Hofle. CERN CAS Darmstadt, October W. Hofle feedback systems

Wolfgang Hofle. CERN CAS Darmstadt, October W. Hofle feedback systems Wolfgang Hofle Wolfgang.Hofle@cern.ch CERN CAS Darmtadt, October 9 Feedback i a mechanim that influence a ytem by looping back an output to the input a concept which i found in abundance in nature and

More information

Stable Soliton Propagation in a System with Spectral Filtering and Nonlinear Gain

Stable Soliton Propagation in a System with Spectral Filtering and Nonlinear Gain  Fiber and Integrated Optic, 19:31] 41, 000 Copyright Q 000 Taylor & Franci 0146-8030 r00 $1.00 q.00 Stable Soliton Propagation in a Sytem with Spectral Filtering and Nonlinear Gain  MARIO F. S. FERREIRA

More information

1. The F-test for Equality of Two Variances

1. The F-test for Equality of Two Variances . The F-tet for Equality of Two Variance Previouly we've learned how to tet whether two population mean are equal, uing data from two independent ample. We can alo tet whether two population variance are

More information

The Laplace Transform , Haynes Miller and Jeremy Orloff

The Laplace Transform , Haynes Miller and Jeremy Orloff The Laplace Tranform 8.3, Hayne Miller and Jeremy Orloff Laplace tranform baic: introduction An operator take a function a input and output another function. A tranform doe the ame thing with the added

More information

Lecture 8: Period Finding: Simon s Problem over Z N

Lecture 8: Period Finding: Simon s Problem over Z N Quantum Computation (CMU 8-859BB, Fall 205) Lecture 8: Period Finding: Simon Problem over Z October 5, 205 Lecturer: John Wright Scribe: icola Rech Problem A mentioned previouly, period finding i a rephraing

More information

Supplementary Figures

Supplementary Figures Supplementary Figure Supplementary Figure S1: Extraction of the SOF. The tandard deviation of meaured V xy at aturated tate (between 2.4 ka/m and 12 ka/m), V 2 d Vxy( H, j, hm ) Vxy( H, j, hm ) 2. The

More information

Fermi Distribution Function. n(e) T = 0 T > 0 E F

Fermi Distribution Function. n(e) T = 0 T > 0 E F LECTURE 3 Maxwell{Boltzmann, Fermi, and Boe Statitic Suppoe we have a ga of N identical point particle in a box ofvolume V. When we ay \ga", we mean that the particle are not interacting with one another.

More information

Fourier-Conjugate Models in the Corpuscular-Wave Dualism Concept

Fourier-Conjugate Models in the Corpuscular-Wave Dualism Concept International Journal of Adanced Reearch in Phyical Science (IJARPS) Volume, Iue 0, October 05, PP 6-30 ISSN 349-7874 (Print) & ISSN 349-788 (Online) www.arcjournal.org Fourier-Conjugate Model in the Corpucular-Wae

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

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

Recent progress in fire-structure analysis

Recent progress in fire-structure analysis EJSE Special Iue: Selected Key Note paper from MDCMS 1 1t International Conference on Modern Deign, Contruction and Maintenance of Structure - Hanoi, Vietnam, December 2007 Recent progre in fire-tructure

More information

Chapter 1 Basic Description of Laser Diode Dynamics by Spatially Averaged Rate Equations: Conditions of Validity

Chapter 1 Basic Description of Laser Diode Dynamics by Spatially Averaged Rate Equations: Conditions of Validity Chapter 1 Baic Decription of Laer Diode Dynamic by Spatially Averaged Rate Equation: Condition of Validity A laer diode i a device in which an electric current input i converted to an output of photon.

More information

Water Analog Experimental Method for the Diffusion and Distribution of Alloy Elements in Liquid Steel during Ingot Filling Process

Water Analog Experimental Method for the Diffusion and Distribution of Alloy Elements in Liquid Steel during Ingot Filling Process , pp. 275 280 Water Analog Experimental Method for the Diffuion and Ditribution of Alloy Element in Liquid Steel during Ingot Filling Proce Jinu KANG, Chao DONG,* Xiaokun HAO, Gang NIE, Houfa SHEN and

More information

IN high performance digital-to-analog converters (DAC),

IN high performance digital-to-analog converters (DAC), A Octuple Sitching Structure ith Code Independent for Frequency Converion of High Performance D/A Converter Wang liguo, Wang zongmin, and Kong ying Abtract A ne itching tructure for decreaing ignal dependent

More information

Standard Guide for Conducting Ruggedness Tests 1

Standard Guide for Conducting Ruggedness Tests 1 Deignation: E 69 89 (Reapproved 996) Standard Guide for Conducting Ruggedne Tet AMERICA SOCIETY FOR TESTIG AD MATERIALS 00 Barr Harbor Dr., Wet Conhohocken, PA 948 Reprinted from the Annual Book of ASTM

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

EP225 Note No. 5 Mechanical Waves

EP225 Note No. 5 Mechanical Waves EP5 Note No. 5 Mechanical Wave 5. Introduction Cacade connection of many ma-pring unit conitute a medium for mechanical wave which require that medium tore both kinetic energy aociated with inertia (ma)

More information

CHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION. Professor Dae Ryook Yang

CHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION. Professor Dae Ryook Yang CHBE3 ECTURE V APACE TRANSFORM AND TRANSFER FUNCTION Profeor Dae Ryook Yang Spring 8 Dept. of Chemical and Biological Engineering 5- Road Map of the ecture V aplace Tranform and Tranfer function Definition

More information