Signals and Systems EE235. Leo Lam

Size: px
Start display at page:

Download "Signals and Systems EE235. Leo Lam"

Transcription

1 Signals and Systems EE35 Leo Lam

2 oday s menu Good weekend? System properties ime invariance (cont ) Linearity Superposition!

3 System properties ime-invariance: A System is ime-invariant if it meets this criterion System Response is the same no matter when you run the system.

4 ime invariance he system behaves the same no matter when you use it If { x( t)} y( t) System st { x( t t )} y( t t ) then 0 0 Input is delayed Systemby t 0 seconds, Delayoutput y(t-t is the 0 ) same but delayed t 0 seconds x(t) Delay st Delay t 0 y(t) x(t-t 0 ) t 0 System = [x(t-t 0 )]

5 ime invariance example Still you (x(t)) = x(5t). y(t) = x(5t). y(t 3) = x(5(t-3)) = x(5t 5) 3. (x(t-3)) = x(5t- 3) 4. Oops Not time invariant! Does it make sense? KEY: In step you replace the t by t-t 0. In step 3 you replace the x(t) by x(t-t 0 ). Shift then scale

6 ime invariance example Graphically: (x(t)) = x(5t). y(t) = x(5t). y(t 3) = x(5(t-3)) = x(5t 5) 3. (x(t-3)) = x(5t- 3) system input x(t) 0 system output y(t) = x(5t) shifted system output y(t-3) = x(5(t-3)) t 0 5 shifted system input x(t-3) t system output for shifted system input (x(t-3)) = x(5t-3) t t t

7 ime invariance example Integral [ x( t)] x( ) d. First:. Second: 3. hird: 4. Lastly: t ime invariant! t y( t) x( ) d tt y( t t0) x( ) d 0 t KEY: In step you replace the t by t-t 0. In step 3 you replace the x(t) by x(t-t 0 ). [ x( t t )] x( t ) d x( v) dv v t tt 0 0 tt tt x( v) dv x( ) d 0

8 System properties Linearity: A System is Linear if it meets the following two criteria: If { x ( t)} y ( t) and { x ( t)} y ( t) hen { x ( t) x ( t)} { x ( t)} { x ( t)} If { x( t)} y( t) hen { ax( t)} a{ x( t)} System Response to a linear combination of inputs is the linear combination of the outputs. ogether superposition Additivity Scaling { ax ( t) bx ( t)} ay ( t) by ( t)

9 Linearity Order of addition and multiplication doesn t matter. System st System y ( t), y ( t) Linear combination ay ( t) by ( t) = x ( t), x ( t) Linear combination ax ( t) bx ( t) System { ax ( t) bx ( t)} Combo st

10 Linearity Positive proof Prove both scaling & additivity separately Prove them together with combined formula Negative proof Show either scaling OR additivity fail (mathematically, or with a counter example) Show combined formula doesn t hold

11 Linearity Proof Combo Proof Step : find y i (t) Step : find y_combo System st System Step 3: find {x_combo} Step 4: If y_combo = {x_combo} Linear y ( t), y ( t) Linear combination ay ( t) by ( t) x ( t), x ( t) Linear combination ax ( t) bx ( t) System { ax ( t) bx ( t)} Combo st

12 Linearity Example Is linear? x(t) y(t)=cx(t) y ( t) cx ( t); y ( t) cx ( t) ay ( t) by ( t) acx ( t) bcx ( t) c( ax ( t) bx ( t)) { ax ( t) bx ( t)} c( ax ( t) bx ( t)) Equal Linear

13 Linearity Example Is linear? x(t) y(t)=(x(t)) y( t) ( x( t)) ay( t) a( x( t)) { ax( t)} ( ax( t)) a ( x( t)) Not equal non-linear

14 Linearity Example Is linear? x(t) y(t)=x(t)+5 y( t) x( t) 5 ay( t) a( x( t) 5) ax( t) 5a { ax( t)} ax( t) 5 Not equal non-linear

15 Linearity Example Is linear? y ( t) x ( t ) d y( t) x( t ) d y ( t) x ( t ) d ay ( t) by ( t) a x ( t ) d b x ( t ) d ( ax ( t ) bx ( t )) d { ax ( t) bx ( t)} ( ax ( t ) bx ( t )) d =

16 Linearity unique case How about scaling with 0? y( t) { x( t)} ay( t) a{ x( t)} 0 if a 0 { ax( t)} ay( t) 0 if linear If {x(t)} is a linear system, then zero input must give a zero output A great negative test

17 Linearity Rules of thumbs multiplying x(t) by another x() y(t)=g[x(t)] where g() is nonlinear piecewise definition of y(t) in terms of values of x, e.g. x( t) x( t) 0 y( t) x( t) x( t) x( t) 0 (although sometimes ok)

18 Superposition Superposition is If x ( t) y ( t) k k x( t) ak xk ( t) y( t) ak yk ( t) k Weighted sum of inputs weighted sum of outputs Divide & conquer k

19 Superposition example Graphically x (t) y (t) x (t) y (t) 3 x ( t) x ( t) y ( t) y ( t) -? y (t) -y (t) 9

20 Superposition example Slightly aside (same system) x (t) y (t) x (t) y (t) 3 Is it time-invariant? No idea: not enough information Single input-output pair cannot test positively 0

21 Superposition example Unique case can be used negatively x (t) x (t) y (t) NO ime Invariant: Shift by shift by y (t) x (t)=u(t) S y (t)=tu(t) NO Stable: Bounded input gives unbounded output

22 Summary: System properties Causal: output does not depend on future input times Invertible: can uniquely find system input for any output Stable: bounded input gives bounded output ime-invariant: ime-shifted input gives a time-shifted output Linear: response to linear combo of inputs is the linear combo of corresponding outputs

4/9/2012. Signals and Systems KX5BQY EE235. Today s menu. System properties

4/9/2012. Signals and Systems   KX5BQY EE235. Today s menu. System properties Signals and Sysems hp://www.youube.com/v/iv6fo KX5BQY EE35 oday s menu Good weeend? Sysem properies iy Superposiion! Sysem properies iy: A Sysem is if i mees he following wo crieria: If { x( )} y( ) and

More information

06/12/ rws/jMc- modif SuFY10 (MPF) - Textbook Section IX 1

06/12/ rws/jMc- modif SuFY10 (MPF) - Textbook Section IX 1 IV. Continuous-Time Signals & LTI Systems [p. 3] Analog signal definition [p. 4] Periodic signal [p. 5] One-sided signal [p. 6] Finite length signal [p. 7] Impulse function [p. 9] Sampling property [p.11]

More information

2. CONVOLUTION. Convolution sum. Response of d.t. LTI systems at a certain input signal

2. CONVOLUTION. Convolution sum. Response of d.t. LTI systems at a certain input signal 2. CONVOLUTION Convolution sum. Response of d.t. LTI systems at a certain input signal Any signal multiplied by the unit impulse = the unit impulse weighted by the value of the signal in 0: xn [ ] δ [

More information

Chapter 1 Fundamental Concepts

Chapter 1 Fundamental Concepts Chapter 1 Fundamental Concepts 1 Signals A signal is a pattern of variation of a physical quantity, often as a function of time (but also space, distance, position, etc). These quantities are usually the

More information

1.17 : Consider a continuous-time system with input x(t) and output y(t) related by y(t) = x( sin(t)).

1.17 : Consider a continuous-time system with input x(t) and output y(t) related by y(t) = x( sin(t)). (Note: here are the solution, only showing you the approach to solve the problems. If you find some typos or calculation error, please post it on Piazza and let us know ).7 : Consider a continuous-time

More information

Chapter 4. Sequential Logic Circuits

Chapter 4. Sequential Logic Circuits Chapter 4 Sequential Logic Circuits 1 2 Chapter 4 4 1 The defining characteristic of a combinational circuit is that its output depends only on the current inputs applied to the circuit. The output of

More information

信號與系統 Signals and Systems

信號與系統 Signals and Systems Spring 2010 信號與系統 Signals and Systems Chapter SS-2 Linear Time-Invariant Systems Feng-Li Lian NTU-EE Feb10 Jun10 Figures and images used in these lecture notes are adopted from Signals & Systems by Alan

More information

Chapter 1 Fundamental Concepts

Chapter 1 Fundamental Concepts Chapter 1 Fundamental Concepts Signals A signal is a pattern of variation of a physical quantity as a function of time, space, distance, position, temperature, pressure, etc. These quantities are usually

More information

Module 1: Signals & System

Module 1: Signals & System Module 1: Signals & System Lecture 6: Basic Signals in Detail Basic Signals in detail We now introduce formally some of the basic signals namely 1) The Unit Impulse function. 2) The Unit Step function

More information

信號與系統 Signals and Systems

信號與系統 Signals and Systems Spring 2015 信號與系統 Signals and Systems Chapter SS-2 Linear Time-Invariant Systems Feng-Li Lian NTU-EE Feb15 Jun15 Figures and images used in these lecture notes are adopted from Signals & Systems by Alan

More information

Classification of Discrete-Time Systems. System Properties. Terminology: Implication. Terminology: Equivalence

Classification of Discrete-Time Systems. System Properties. Terminology: Implication. Terminology: Equivalence Classification of Discrete-Time Systems Professor Deepa Kundur University of Toronto Why is this so important? mathematical techniques developed to analyze systems are often contingent upon the general

More information

New Mexico State University Klipsch School of Electrical Engineering. EE312 - Signals and Systems I Fall 2017 Exam #1

New Mexico State University Klipsch School of Electrical Engineering. EE312 - Signals and Systems I Fall 2017 Exam #1 New Mexico State University Klipsch School of Electrical Engineering EE312 - Signals and Systems I Fall 2017 Exam #1 Name: Prob. 1 Prob. 2 Prob. 3 Prob. 4 Total / 30 points / 20 points / 25 points / 25

More information

ECE 301 Division 1 Exam 1 Solutions, 10/6/2011, 8-9:45pm in ME 1061.

ECE 301 Division 1 Exam 1 Solutions, 10/6/2011, 8-9:45pm in ME 1061. ECE 301 Division 1 Exam 1 Solutions, 10/6/011, 8-9:45pm in ME 1061. Your ID will be checked during the exam. Please bring a No. pencil to fill out the answer sheet. This is a closed-book exam. No calculators

More information

1.4 Unit Step & Unit Impulse Functions

1.4 Unit Step & Unit Impulse Functions 1.4 Unit Step & Unit Impulse Functions 1.4.1 The Discrete-Time Unit Impulse and Unit-Step Sequences Unit Impulse Function: δ n = ቊ 0, 1, n 0 n = 0 Figure 1.28: Discrete-time Unit Impulse (sample) 1 [n]

More information

Chapter 3. Discrete-Time Systems

Chapter 3. Discrete-Time Systems Chapter 3 Discrete-Time Systems A discrete-time system can be thought of as a transformation or operator that maps an input sequence {x[n]} to an output sequence {y[n]} {x[n]} T(. ) {y[n]} By placing various

More information

MAHALAKSHMI ENGINEERING COLLEGE-TRICHY

MAHALAKSHMI ENGINEERING COLLEGE-TRICHY DIGITAL SIGNAL PROCESSING UNIT-I PART-A DEPT. / SEM.: CSE/VII. Define a causal system? AUC APR 09 The causal system generates the output depending upon present and past inputs only. A causal system is

More information

EE 341 Homework Chapter 2

EE 341 Homework Chapter 2 EE 341 Homework Chapter 2 2.1 The electrical circuit shown in Fig. P2.1 consists of two resistors R1 and R2 and a capacitor C. Determine the differential equation relating the input voltage v(t) to the

More information

The Convolution Sum for Discrete-Time LTI Systems

The Convolution Sum for Discrete-Time LTI Systems The Convolution Sum for Discrete-Time LTI Systems Andrew W. H. House 01 June 004 1 The Basics of the Convolution Sum Consider a DT LTI system, L. x(n) L y(n) DT convolution is based on an earlier result

More information

10/10/2011. Signals and Systems EE235. Today s menu. Chicken

10/10/2011. Signals and Systems EE235. Today s menu. Chicken Signals and Sysems EE35 Today s menu Homework 1 Due omorrow Ocober 14 h Lecure will be online Sysem properies Lineariy Time invariance Sabiliy Inveribiliy Causaliy Los of examples! Chicken Why did he chicken

More information

/ / MET Day 000 NC1^ INRTL MNVR I E E PRE SLEEP K PRE SLEEP R E

/ / MET Day 000 NC1^ INRTL MNVR I E E PRE SLEEP K PRE SLEEP R E 05//0 5:26:04 09/6/0 (259) 6 7 8 9 20 2 22 2 09/7 0 02 0 000/00 0 02 0 04 05 06 07 08 09 0 2 ay 000 ^ 0 X Y / / / / ( %/ ) 2 /0 2 ( ) ^ 4 / Y/ 2 4 5 6 7 8 9 2 X ^ X % 2 // 09/7/0 (260) ay 000 02 05//0

More information

Basic concepts in DT systems. Alexandra Branzan Albu ELEC 310-Spring 2009-Lecture 4 1

Basic concepts in DT systems. Alexandra Branzan Albu ELEC 310-Spring 2009-Lecture 4 1 Basic concepts in DT systems Alexandra Branzan Albu ELEC 310-Spring 2009-Lecture 4 1 Readings and homework For DT systems: Textbook: sections 1.5, 1.6 Suggested homework: pp. 57-58: 1.15 1.16 1.18 1.19

More information

Signals and Systems Chapter 2

Signals and Systems Chapter 2 Signals and Systems Chapter 2 Continuous-Time Systems Prof. Yasser Mostafa Kadah Overview of Chapter 2 Systems and their classification Linear time-invariant systems System Concept Mathematical transformation

More information

Lecture 1: Introduction Introduction

Lecture 1: Introduction Introduction Module 1: Signals in Natural Domain Lecture 1: Introduction Introduction The intent of this introduction is to give the reader an idea about Signals and Systems as a field of study and its applications.

More information

Lecture 2. Introduction to Systems (Lathi )

Lecture 2. Introduction to Systems (Lathi ) Lecture 2 Introduction to Systems (Lathi 1.6-1.8) Pier Luigi Dragotti Department of Electrical & Electronic Engineering Imperial College London URL: www.commsp.ee.ic.ac.uk/~pld/teaching/ E-mail: p.dragotti@imperial.ac.uk

More information

Identification Methods for Structural Systems

Identification Methods for Structural Systems Prof. Dr. Eleni Chatzi System Stability Fundamentals Overview System Stability Assume given a dynamic system with input u(t) and output x(t). The stability property of a dynamic system can be defined from

More information

Math Lecture 18 Notes

Math Lecture 18 Notes Math 1010 - Lecture 18 Notes Dylan Zwick Fall 2009 In our last lecture we talked about how we can add, subtract, and multiply polynomials, and we figured out that, basically, if you can add, subtract,

More information

Step 1. Step 2. Step 4. The corrected trial solution y with evaluated coefficients d 1, d 2,..., d k becomes the particular solution y p.

Step 1. Step 2. Step 4. The corrected trial solution y with evaluated coefficients d 1, d 2,..., d k becomes the particular solution y p. Definition Atoms A and B are related if and only if their successive derivatives share a common atom. Then x 3 is related to x and x 101, while x is unrelated to e x, xe x and x sin x. Atoms x sin x and

More information

III. Time Domain Analysis of systems

III. Time Domain Analysis of systems 1 III. Time Domain Analysis of systems Here, we adapt properties of continuous time systems to discrete time systems Section 2.2-2.5, pp 17-39 System Notation y(n) = T[ x(n) ] A. Types of Systems Memoryless

More information

Last lecture: Recurrence relations and differential equations. The solution to the differential equation dx

Last lecture: Recurrence relations and differential equations. The solution to the differential equation dx Last lecture: Recurrence relations and differential equations The solution to the differential equation dx = ax is x(t) = ce ax, where c = x() is determined by the initial conditions x(t) Let X(t) = and

More information

Vector Spaces and Subspaces

Vector Spaces and Subspaces Vector Spaces and Subspaces Vector Space V Subspaces S of Vector Space V The Subspace Criterion Subspaces are Working Sets The Kernel Theorem Not a Subspace Theorem Independence and Dependence in Abstract

More information

EE361: Signals and System II

EE361: Signals and System II Professor Brendan Morris, SEB 3216, brendan.morris@unlv.edu EE361: Signals and System II Introduction http://www.ee.unlv.edu/~b1morris/ee361/ 2 Class Website http://www.ee.unlv.edu/~b1morris/ee361/ This

More information

CDS Solutions to the Midterm Exam

CDS Solutions to the Midterm Exam CDS 22 - Solutions to the Midterm Exam Instructor: Danielle C. Tarraf November 6, 27 Problem (a) Recall that the H norm of a transfer function is time-delay invariant. Hence: ( ) Ĝ(s) = s + a = sup /2

More information

2t t dt.. So the distance is (t2 +6) 3/2

2t t dt.. So the distance is (t2 +6) 3/2 Math 8, Solutions to Review for the Final Exam Question : The distance is 5 t t + dt To work that out, integrate by parts with u t +, so that t dt du The integral is t t + dt u du u 3/ (t +) 3/ So the

More information

Nonlinear Control. Nonlinear Control Lecture # 6 Passivity and Input-Output Stability

Nonlinear Control. Nonlinear Control Lecture # 6 Passivity and Input-Output Stability Nonlinear Control Lecture # 6 Passivity and Input-Output Stability Passivity: Memoryless Functions y y y u u u (a) (b) (c) Passive Passive Not passive y = h(t,u), h [0, ] Vector case: y = h(t,u), h T =

More information

3. Frequency-Domain Analysis of Continuous- Time Signals and Systems

3. Frequency-Domain Analysis of Continuous- Time Signals and Systems 3. Frequency-Domain Analysis of Continuous- ime Signals and Systems 3.. Definition of Continuous-ime Fourier Series (3.3-3.4) 3.2. Properties of Continuous-ime Fourier Series (3.5) 3.3. Definition of Continuous-ime

More information

EE 380. Linear Control Systems. Lecture 10

EE 380. Linear Control Systems. Lecture 10 EE 380 Linear Control Systems Lecture 10 Professor Jeffrey Schiano Department of Electrical Engineering Lecture 10. 1 Lecture 10 Topics Stability Definitions Methods for Determining Stability Lecture 10.

More information

Ch 2: Linear Time-Invariant System

Ch 2: Linear Time-Invariant System Ch 2: Linear Time-Invariant System A system is said to be Linear Time-Invariant (LTI) if it possesses the basic system properties of linearity and time-invariance. Consider a system with an output signal

More information

6/27/2012. Signals and Systems EE235. Chicken. Today s menu. Why did the chicken cross the Möbius Strip? To get to the other er um

6/27/2012. Signals and Systems EE235. Chicken. Today s menu. Why did the chicken cross the Möbius Strip? To get to the other er um Signals and Sysems EE35 Chicken Why did he chicken cross he Möbius Srip? To ge o he oher er um Today s menu Sysem properies Lineariy Time invariance Sabiliy Inveribiliy Causaliy Los of examples! 1 Sysem

More information

Math 310 Introduction to Ordinary Differential Equations Final Examination August 9, Instructor: John Stockie

Math 310 Introduction to Ordinary Differential Equations Final Examination August 9, Instructor: John Stockie Make sure this exam has 15 pages. Math 310 Introduction to Ordinary Differential Equations inal Examination August 9, 2006 Instructor: John Stockie Name: (Please Print) Student Number: Special Instructions

More information

Solving Dynamic Equations: The State Transition Matrix

Solving Dynamic Equations: The State Transition Matrix Overview Solving Dynamic Equations: The State Transition Matrix EGR 326 February 24, 2017 Solutions to coupled dynamic equations Solutions to dynamic circuits from EGR 220 The state transition matrix Discrete

More information

CIS 4930/6930: Principles of Cyber-Physical Systems

CIS 4930/6930: Principles of Cyber-Physical Systems CIS 4930/6930: Principles of Cyber-Physical Systems Chapter 2: Continuous Dynamics Hao Zheng Department of Computer Science and Engineering University of South Florida H. Zheng (CSE USF) CIS 4930/6930:

More information

Solutions of Chapter 3 Part 1/2

Solutions of Chapter 3 Part 1/2 Page 1 of 7 Solutions of Chapter 3 Part 1/ Problem 3.1-1 Find the energy of the signals depicted in Figs.P3.1-1. Figure 1: Fig3.1-1 (a) E x n x[n] 1 + + 3 + + 1 19 (b) E x n x[n] 1 + + 3 + + 1 19 (c) E

More information

EE123 Digital Signal Processing

EE123 Digital Signal Processing EE123 Digital Signal Processing Lecture 2A D.T Systems D. T. Fourier Transform A couple of things Read Ch 2 2.0-2.9 It s OK to use 2nd edition My office hours: posted on-line W 4-5pm Cory 506 ham radio

More information

Digital Signal Processing Lecture 4

Digital Signal Processing Lecture 4 Remote Sensing Laboratory Dept. of Information Engineering and Computer Science University of Trento Via Sommarive, 14, I-38123 Povo, Trento, Italy Digital Signal Processing Lecture 4 Begüm Demir E-mail:

More information

New Mexico State University Klipsch School of Electrical Engineering. EE312 - Signals and Systems I Spring 2018 Exam #1

New Mexico State University Klipsch School of Electrical Engineering. EE312 - Signals and Systems I Spring 2018 Exam #1 New Mexico State University Klipsch School of Electrical Engineering EE312 - Signals and Systems I Spring 2018 Exam #1 Name: Prob. 1 Prob. 2 Prob. 3 Prob. 4 Total / 30 points / 20 points / 25 points /

More information

Noise - irrelevant data; variability in a quantity that has no meaning or significance. In most cases this is modeled as a random variable.

Noise - irrelevant data; variability in a quantity that has no meaning or significance. In most cases this is modeled as a random variable. 1.1 Signals and Systems Signals convey information. Systems respond to (or process) information. Engineers desire mathematical models for signals and systems in order to solve design problems efficiently

More information

Sequential Logic Circuits

Sequential Logic Circuits Chapter 4 Sequential Logic Circuits 4 1 The defining characteristic of a combinational circuit is that its output depends only on the current inputs applied to the circuit. The output of a sequential circuit,

More information

Time Series Analysis

Time Series Analysis Time Series Analysis Informatics and Mathematical Modelling Technical University of Denmark DK-2800 Kgs. Lyngby 1 Outline of todays lecture Descriptions of (deterministic) linear systems. Chapter 4: Linear

More information

Linear dynamical systems with inputs & outputs

Linear dynamical systems with inputs & outputs EE263 Autumn 215 S. Boyd and S. Lall Linear dynamical systems with inputs & outputs inputs & outputs: interpretations transfer function impulse and step responses examples 1 Inputs & outputs recall continuous-time

More information

x 9 or x > 10 Name: Class: Date: 1 How many natural numbers are between 1.5 and 4.5 on the number line?

x 9 or x > 10 Name: Class: Date: 1 How many natural numbers are between 1.5 and 4.5 on the number line? 1 How many natural numbers are between 1.5 and 4.5 on the number line? 2 How many composite numbers are between 7 and 13 on the number line? 3 How many prime numbers are between 7 and 20 on the number

More information

Therefore the new Fourier coefficients are. Module 2 : Signals in Frequency Domain Problem Set 2. Problem 1

Therefore the new Fourier coefficients are. Module 2 : Signals in Frequency Domain Problem Set 2. Problem 1 Module 2 : Signals in Frequency Domain Problem Set 2 Problem 1 Let be a periodic signal with fundamental period T and Fourier series coefficients. Derive the Fourier series coefficients of each of the

More information

6.02 Fall 2012 Lecture #10

6.02 Fall 2012 Lecture #10 6.02 Fall 2012 Lecture #10 Linear time-invariant (LTI) models Convolution 6.02 Fall 2012 Lecture 10, Slide #1 Modeling Channel Behavior codeword bits in generate x[n] 1001110101 digitized modulate DAC

More information

Continuous Dynamics Solving LTI state-space equations גרא וייס המחלקה למדעי המחשב אוניברסיטת בן-גוריון

Continuous Dynamics Solving LTI state-space equations גרא וייס המחלקה למדעי המחשב אוניברסיטת בן-גוריון Continuous Dynamics Solving LTI state-space equations גרא וייס המחלקה למדעי המחשב אוניברסיטת בן-גוריון 2 State Space Models For a causal system with m inputs u t R m and p outputs y t R p, an nth-order

More information

Understanding the Matrix Exponential

Understanding the Matrix Exponential Transformations Understanding the Matrix Exponential Lecture 8 Math 634 9/17/99 Now that we have a representation of the solution of constant-coefficient initial-value problems, we should ask ourselves:

More information

Linear Algebra and Matrix Inversion

Linear Algebra and Matrix Inversion Jim Lambers MAT 46/56 Spring Semester 29- Lecture 2 Notes These notes correspond to Section 63 in the text Linear Algebra and Matrix Inversion Vector Spaces and Linear Transformations Matrices are much

More information

Equilibrium points: continuous-time systems

Equilibrium points: continuous-time systems Capitolo 0 INTRODUCTION 81 Equilibrium points: continuous-time systems Let us consider the following continuous-time linear system ẋ(t) Ax(t)+Bu(t) y(t) Cx(t)+Du(t) The equilibrium points x 0 of the system

More information

On the Global Existence of Solutions to a System of Second Order Nonlinear Differential Equations

On the Global Existence of Solutions to a System of Second Order Nonlinear Differential Equations On the Global Existence of Solutions to a System of Second Order Nonlinear Differential Equations Faniran aye Samuel Department of Computer Science, Lead City University, Ibadan. P.O.Box 3678, Secretariat,

More information

Lecture 2 ELE 301: Signals and Systems

Lecture 2 ELE 301: Signals and Systems Lecture 2 ELE 301: Signals and Systems Prof. Paul Cuff Princeton University Fall 2011-12 Cuff (Lecture 2) ELE 301: Signals and Systems Fall 2011-12 1 / 70 Models of Continuous Time Signals Today s topics:

More information

Analog Signals and Systems and their properties

Analog Signals and Systems and their properties Analog Signals and Systems and their properties Main Course Objective: Recall course objectives Understand the fundamentals of systems/signals interaction (know how systems can transform or filter signals)

More information

Dynamical systems: basic concepts

Dynamical systems: basic concepts Dynamical systems: basic concepts Daniele Carnevale Dipartimento di Ing. Civile ed Ing. Informatica (DICII), University of Rome Tor Vergata Fondamenti di Automatica e Controlli Automatici A.A. 2014-2015

More information

Lyapunov Stability Analysis: Open Loop

Lyapunov Stability Analysis: Open Loop Copyright F.L. Lewis 008 All rights reserved Updated: hursday, August 8, 008 Lyapunov Stability Analysis: Open Loop We know that the stability of linear time-invariant (LI) dynamical systems can be determined

More information

Digital Signal Processing, Homework 1, Spring 2013, Prof. C.D. Chung

Digital Signal Processing, Homework 1, Spring 2013, Prof. C.D. Chung Digital Signal Processing, Homework, Spring 203, Prof. C.D. Chung. (0.5%) Page 99, Problem 2.2 (a) The impulse response h [n] of an LTI system is known to be zero, except in the interval N 0 n N. The input

More information

VU Signal and Image Processing

VU Signal and Image Processing 052600 VU Signal and Image Processing Torsten Möller + Hrvoje Bogunović + Raphael Sahann torsten.moeller@univie.ac.at hrvoje.bogunovic@meduniwien.ac.at raphael.sahann@univie.ac.at vda.cs.univie.ac.at/teaching/sip/18s/

More information

Section 2.1 (First Order) Linear DEs; Method of Integrating Factors. General first order linear DEs Standard Form; y'(t) + p(t) y = g(t)

Section 2.1 (First Order) Linear DEs; Method of Integrating Factors. General first order linear DEs Standard Form; y'(t) + p(t) y = g(t) Section 2.1 (First Order) Linear DEs; Method of Integrating Factors Key Terms/Ideas: General first order linear DEs Standard Form; y'(t) + p(t) y = g(t) Integrating factor; a function μ(t) that transforms

More information

Basic Theory of Linear Differential Equations

Basic Theory of Linear Differential Equations Basic Theory of Linear Differential Equations Picard-Lindelöf Existence-Uniqueness Vector nth Order Theorem Second Order Linear Theorem Higher Order Linear Theorem Homogeneous Structure Recipe for Constant-Coefficient

More information

Lecture 7: September 17

Lecture 7: September 17 10-725: Optimization Fall 2013 Lecture 7: September 17 Lecturer: Ryan Tibshirani Scribes: Serim Park,Yiming Gu 7.1 Recap. The drawbacks of Gradient Methods are: (1) requires f is differentiable; (2) relatively

More information

EL1820 Modeling of Dynamical Systems

EL1820 Modeling of Dynamical Systems EL1820 Modeling of Dynamical Systems Lecture 10 - System identification as a model building tool Experiment design Examination and prefiltering of data Model structure selection Model validation Lecture

More information

Shift Property of z-transform. Lecture 16. More z-transform (Lathi 5.2, ) More Properties of z-transform. Convolution property of z-transform

Shift Property of z-transform. Lecture 16. More z-transform (Lathi 5.2, ) More Properties of z-transform. Convolution property of z-transform Shift Property of -Transform If Lecture 6 More -Transform (Lathi 5.2,5.4-5.5) then which is delay causal signal by sample period. If we delay x[n] first: Peter Cheung Department of Electrical & Electronic

More information

Problem Set 1 Solutions

Problem Set 1 Solutions Introduction to Algorithms September 24, 2004 Massachusetts Institute of Technology 6.046J/18.410J Professors Piotr Indyk and Charles E. Leiserson Handout 7 Problem Set 1 Solutions Exercise 1-1. Do Exercise

More information

(the matrix with b 1 and b 2 as columns). If x is a vector in R 2, then its coordinate vector [x] B relative to B satisfies the formula.

(the matrix with b 1 and b 2 as columns). If x is a vector in R 2, then its coordinate vector [x] B relative to B satisfies the formula. 4 Diagonalization 4 Change of basis Let B (b,b ) be an ordered basis for R and let B b b (the matrix with b and b as columns) If x is a vector in R, then its coordinate vector x B relative to B satisfies

More information

P3.C8.COMPLEX NUMBERS

P3.C8.COMPLEX NUMBERS Recall: Within the real number system, we can solve equation of the form and b 2 4ac 0. ax 2 + bx + c =0, where a, b, c R What is R? They are real numbers on the number line e.g: 2, 4, π, 3.167, 2 3 Therefore,

More information

THE RING OF POLYNOMIALS. Special Products and Factoring

THE RING OF POLYNOMIALS. Special Products and Factoring THE RING OF POLYNOMIALS Special Products and Factoring Special Products and Factoring Upon completion, you should be able to Find special products Factor a polynomial completely Special Products - rules

More information

Homework 3 Solutions

Homework 3 Solutions 18-290 Signals and Systems Profs. Byron Yu and Pulkit Grover Fall 2018 Homework 3 Solutions Part One 1. (25 points) The following systems have x(t) or x[n] as input and y(t) or y[n] as output. For each

More information

Theorem 1. ẋ = Ax is globally exponentially stable (GES) iff A is Hurwitz (i.e., max(re(σ(a))) < 0).

Theorem 1. ẋ = Ax is globally exponentially stable (GES) iff A is Hurwitz (i.e., max(re(σ(a))) < 0). Linear Systems Notes Lecture Proposition. A M n (R) is positive definite iff all nested minors are greater than or equal to zero. n Proof. ( ): Positive definite iff λ i >. Let det(a) = λj and H = {x D

More information

EECE 3620: Linear Time-Invariant Systems: Chapter 2

EECE 3620: Linear Time-Invariant Systems: Chapter 2 EECE 3620: Linear Time-Invariant Systems: Chapter 2 Prof. K. Chandra ECE, UMASS Lowell September 7, 2016 1 Continuous Time Systems In the context of this course, a system can represent a simple or complex

More information

STEP Support Programme. Hints and Partial Solutions for Assignment 1

STEP Support Programme. Hints and Partial Solutions for Assignment 1 STEP Support Programme Hints and Partial Solutions for Assignment 1 Warm-up 1 You can check many of your answers to this question by using Wolfram Alpha. Only use this as a check though and if your answer

More information

Nonlinear Control Lecture # 1 Introduction. Nonlinear Control

Nonlinear Control Lecture # 1 Introduction. Nonlinear Control Nonlinear Control Lecture # 1 Introduction Nonlinear State Model ẋ 1 = f 1 (t,x 1,...,x n,u 1,...,u m ) ẋ 2 = f 2 (t,x 1,...,x n,u 1,...,u m ).. ẋ n = f n (t,x 1,...,x n,u 1,...,u m ) ẋ i denotes the derivative

More information

Section 1.4: Second-Order and Higher-Order Equations. Consider a second-order, linear, homogeneous equation with constant coefficients

Section 1.4: Second-Order and Higher-Order Equations. Consider a second-order, linear, homogeneous equation with constant coefficients Section 1.4: Second-Order and Higher-Order Equations Consider a second-order, linear, homogeneous equation with constant coefficients x t+2 + ax t+1 + bx t = 0. (1) To solve this difference equation, we

More information

6.241 Dynamic Systems and Control

6.241 Dynamic Systems and Control 6.241 Dynamic Systems and Control Lecture 8: Solutions of State-space Models Readings: DDV, Chapters 10, 11, 12 (skip the parts on transform methods) Emilio Frazzoli Aeronautics and Astronautics Massachusetts

More information

7.3 Singular points and the method of Frobenius

7.3 Singular points and the method of Frobenius 284 CHAPTER 7. POWER SERIES METHODS 7.3 Singular points and the method of Frobenius Note: or.5 lectures, 8.4 and 8.5 in [EP], 5.4 5.7 in [BD] While behaviour of ODEs at singular points is more complicated,

More information

Vector Spaces and Subspaces

Vector Spaces and Subspaces Vector Spaces and Subspaces Vector Space V Subspaces S of Vector Space V The Subspace Criterion Subspaces are Working Sets The Kernel Theorem Not a Subspace Theorem Independence and Dependence in Abstract

More information

1. FIR Filter Design

1. FIR Filter Design ELEN E4810: Digital Signal Processing Topic 9: Filter Design: FIR 1. Windowed Impulse Response 2. Window Shapes 3. Design by Iterative Optimization 1 1. FIR Filter Design! FIR filters! no poles (just zeros)!

More information

Maple Output Maple Plot 2D Math 2D Output

Maple Output Maple Plot 2D Math 2D Output Maple Output Maple Plot 2D Math 2D Output 0.1 Introduction Vectors 1 On one level a vector is just a point; we can regard every point in R 2 as a vector. When we do so we will write a, b instead of the

More information

34.3. Resisted Motion. Introduction. Prerequisites. Learning Outcomes

34.3. Resisted Motion. Introduction. Prerequisites. Learning Outcomes Resisted Motion 34.3 Introduction This Section returns to the simple models of projectiles considered in Section 34.1. It explores the magnitude of air resistance effects and the effects of including simple

More information

The Corrected Trial Solution in the Method of Undetermined Coefficients

The Corrected Trial Solution in the Method of Undetermined Coefficients Definition of Related Atoms The Basic Trial Solution Method Symbols Superposition Annihilator Polynomial for f(x) Annihilator Equation for f(x) The Corrected Trial Solution in the Method of Undetermined

More information

Examples 2: Composite Functions, Piecewise Functions, Partial Fractions

Examples 2: Composite Functions, Piecewise Functions, Partial Fractions Examples 2: Composite Functions, Piecewise Functions, Partial Fractions September 26, 206 The following are a set of examples to designed to complement a first-year calculus course. objectives are listed

More information

1+t 2 (l) y = 2xy 3 (m) x = 2tx + 1 (n) x = 2tx + t (o) y = 1 + y (p) y = ty (q) y =

1+t 2 (l) y = 2xy 3 (m) x = 2tx + 1 (n) x = 2tx + t (o) y = 1 + y (p) y = ty (q) y = DIFFERENTIAL EQUATIONS. Solved exercises.. Find the set of all solutions of the following first order differential equations: (a) x = t (b) y = xy (c) x = x (d) x = (e) x = t (f) x = x t (g) x = x log

More information

ENT 315 Medical Signal Processing CHAPTER 2 DISCRETE FOURIER TRANSFORM. Dr. Lim Chee Chin

ENT 315 Medical Signal Processing CHAPTER 2 DISCRETE FOURIER TRANSFORM. Dr. Lim Chee Chin ENT 315 Medical Signal Processing CHAPTER 2 DISCRETE FOURIER TRANSFORM Dr. Lim Chee Chin Outline Introduction Discrete Fourier Series Properties of Discrete Fourier Series Time domain aliasing due to frequency

More information

Absolute Value Equations and Inequalities. Use the distance definition of absolute value.

Absolute Value Equations and Inequalities. Use the distance definition of absolute value. Chapter 2 Section 7 2.7 Absolute Value Equations and Inequalities Objectives 1 2 3 4 5 6 Use the distance definition of absolute value. Solve equations of the form ax + b = k, for k > 0. Solve inequalities

More information

Full file at 2CT IMPULSE, IMPULSE RESPONSE, AND CONVOLUTION CHAPTER 2CT

Full file at   2CT IMPULSE, IMPULSE RESPONSE, AND CONVOLUTION CHAPTER 2CT 2CT.2 UNIT IMPULSE 2CT.2. CHAPTER 2CT 2CT.2.2 (d) We can see from plot (c) that the limit?7 Ä!, B :?7 9 œb 9$ 9. This result is consistent with the sampling property: B $ œb $ 9 9 9 9 2CT.2.3 # # $ sin

More information

NAME DATE PERIOD. Study Guide and Intervention. Solving Polynomial Equations. For any number of terms, check for: greatest common factor

NAME DATE PERIOD. Study Guide and Intervention. Solving Polynomial Equations. For any number of terms, check for: greatest common factor 5-5 Factor Polynomials Study Guide and Intervention For any number of terms, check for: greatest common factor Techniques for Factoring Polynomials For two terms, check for: Difference of two squares a

More information

Nonlinear Control Lecture 7: Passivity

Nonlinear Control Lecture 7: Passivity Nonlinear Control Lecture 7: Passivity Farzaneh Abdollahi Department of Electrical Engineering Amirkabir University of Technology Fall 2011 Farzaneh Abdollahi Nonlinear Control Lecture 7 1/26 Passivity

More information

6.241 Dynamic Systems and Control

6.241 Dynamic Systems and Control 6.241 Dynamic Systems and Control Lecture 7: State-space Models Readings: DDV, Chapters 7,8 Emilio Frazzoli Aeronautics and Astronautics Massachusetts Institute of Technology February 25, 2011 E. Frazzoli

More information

GATE EE Topic wise Questions SIGNALS & SYSTEMS

GATE EE Topic wise Questions SIGNALS & SYSTEMS www.gatehelp.com GATE EE Topic wise Questions YEAR 010 ONE MARK Question. 1 For the system /( s + 1), the approximate time taken for a step response to reach 98% of the final value is (A) 1 s (B) s (C)

More information

NAME: 13 February 2013 EE301 Signals and Systems Exam 1 Cover Sheet

NAME: 13 February 2013 EE301 Signals and Systems Exam 1 Cover Sheet NAME: February EE Signals and Systems Exam Cover Sheet Test Duration: 75 minutes. Coverage: Chaps., Open Book but Closed Notes. One 8.5 in. x in. crib sheet Calculators NOT allowed. This test contains

More information

Permutations and Polynomials Sarah Kitchen February 7, 2006

Permutations and Polynomials Sarah Kitchen February 7, 2006 Permutations and Polynomials Sarah Kitchen February 7, 2006 Suppose you are given the equations x + y + z = a and 1 x + 1 y + 1 z = 1 a, and are asked to prove that one of x,y, and z is equal to a. We

More information

Solving Dynamic Equations: The State Transition Matrix II

Solving Dynamic Equations: The State Transition Matrix II Reading the Text Solving Dynamic Equations: The State Transition Matrix II EGR 326 February 27, 2017 Just a reminder to read the text Read through longer passages, to see what is connected to class topics.

More information

EEE 303 Notes: System properties

EEE 303 Notes: System properties EEE 303 Notes: System properties Kostas Tsakalis January 27, 2000 1 Introduction The purpose of this note is to provide a brief background and some examples on the fundamental system properties. In particular,

More information

Lesson 3: Linear differential equations of the first order Solve each of the following differential equations by two methods.

Lesson 3: Linear differential equations of the first order Solve each of the following differential equations by two methods. Lesson 3: Linear differential equations of the first der Solve each of the following differential equations by two methods. Exercise 3.1. Solution. Method 1. It is clear that y + y = 3 e dx = e x is an

More information

SOLUTIONS TO ECE 3084

SOLUTIONS TO ECE 3084 SOLUTIONS TO ECE 384 PROBLEM 2.. For each sysem below, specify wheher or no i is: (i) memoryless; (ii) causal; (iii) inverible; (iv) linear; (v) ime invarian; Explain your reasoning. If he propery is no

More information