The Continuous Time Fourier Transform

Size: px
Start display at page:

Download "The Continuous Time Fourier Transform"

Transcription

1 COMM 401: Signals & Systems Theory Lecture 8 The Continuous Time Fourier Transform

2 Fourier Transform Continuous time CT signals Discrete time DT signals Aperiodic signals nonperiodic periodic signals Aperiodic signals nonperiodic periodic signals

3 Fourier Representation of Signals

4 Development of FT of an aperiodic signal

5 Continuous Time Fourier Transform The previous equation can be seen as samples of an envelope function as: Let k0 2sin T / represents the envelope of coefficients Envelope With thought of as a continuous variable, the function 1 a k Ta and the are simply equally spacedsamples of this envelope k

6 Continuous Time Fourier Transform ~ the set of F.S Coefficients approaches the Envelope function

7 Derivation of Continuous Time Fourier Transform Envelope

8 Fourier Transform & Inverse FT use T 2 0

9 T 2 0

10 Conditions of Convergence of FT Convergence is guaranteed if xt satisfies the following conditions for non-periodic signals:

11 Example: Analog Signals Fourier Transform

12 Remember: The sinc function

13 Example : Determine the FT of the signal? Famous Signal

14 Example: Solution As W increases the width main lobe of x t becomes narrower and the main peak becomes higher. of

15 Example: Determine the FT of the signal? a > 0 Famous Signal Draw the magnitude and phase of FT of the signal.

16 Example: Magnitude Response Phase Response

17 Example: Determine the FT of the signal? Famous Signal 1

18 Example: Determine the IFT of the signal?

19 Properties of the Continuous Time FT Remarks

20 Example: Determine the FT of the signal? 1

21 Properties of the Continuous Time FT Time Scale

22 Properties of the Continuous Time FT xt = x ev t + x od t and hence, Example: x t X j Ev Od x t ReX j x t j ImX j Famous Signal

23

24 Properties of the Continuous Time FT

25 Properties of the Continuous Time FT

26 Example:

27 Properties of the Continuous Time FT

28 Properties of the Continuous Time FT xt X j LTIS ht H j yt Y j Convolution Property: yt ht*xt F.T Y j H j X j Example : Consider a LTIS with impulse responseh t : Then the output of the system in the time domain is : y t x t* h t and in the frequency domain : Y j H j X j Important

29 Example: , 1 1 Solution input the to response: impulse system with a of output the Find t u e e t u e t u e t y j j j B j A j j j Y j j X j j H j X j H j Y t u e t x t u e t h t t t t t t Important

30 Properties of the Continuous Time FT Duality: By comparing the F.T and the inverse F.T equations, we observe that these equations are similar but not identical in form. This symmetry leads to a property of the F.T referred to as duality. Example:

31 Specifically, because of the symmetry between F.T and IFT Equations for any transform pair, there is a dual pair with the time and frequency variables interchanged. We saw that differentiation in the time domain corresponds to multiplication by in the frequency domain. Then, multiplication by -jt in the time domain corresponds roughly to differentiation in the frequency domain. If we differentiate the Fourier transform equation w.r.t : X dx j d Then; j x t e jtx t jt dt jtx t e FT jt dt dx j d

32 Properties of the Continuous Time FT Similar to Time shifting Property Similar to Integration Property j X e t t x o t j FT o 0 1 X j X j d x t Similar to differentiation Property Frequency domain Multiplication Property: ] [ 2 1 j P j S j R t p t s t r

33 Example: t zt=xt j a j 2

34 Frequency Shaping and Filtering Frequency Response: e j

35 Frequency Shaping and Filtering

36 Frequency Shaping and Filtering

37 Frequency Response and Filtering

38 Frequency Response and Filtering

39 Practical Example: Remember Frequency Response and Filtering a 1 RC

40 Frequency Response and Filtering

41 Properties of the Continuous Time FT Convolution property: h1 t h2 t H1 j H 2 j

42 Frequency Response and Filtering

43 Example: The frequency response of this system is the Fourier transform of its impulse response which is given by: Then, for any input xt, the Fourier Transform of the output is given by: In time domain and using time shifting property, yt is given by:

44 Example:

Continuous-Time Fourier Transform

Continuous-Time Fourier Transform Signals and Systems Continuous-Time Fourier Transform Chang-Su Kim continuous time discrete time periodic (series) CTFS DTFS aperiodic (transform) CTFT DTFT Lowpass Filtering Blurring or Smoothing Original

More information

Ch 4: The Continuous-Time Fourier Transform

Ch 4: The Continuous-Time Fourier Transform Ch 4: The Continuous-Time Fourier Transform Fourier Transform of x(t) Inverse Fourier Transform jt X ( j) x ( t ) e dt jt x ( t ) X ( j) e d 2 Ghulam Muhammad, King Saud University Continuous-time aperiodic

More information

The Continuous-time Fourier

The Continuous-time Fourier The Continuous-time Fourier Transform Rui Wang, Assistant professor Dept. of Information and Communication Tongji University it Email: ruiwang@tongji.edu.cn Outline Representation of Aperiodic signals:

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

信號與系統 Signals and Systems

信號與系統 Signals and Systems Spring 2011 信號與系統 Signals and Systems Chapter SS-4 The Continuous-Time Fourier Transform Feng-Li Lian NTU-EE Feb11 Jun11 Figures and images used in these lecture notes are adopted from Signals & Systems

More information

Notes 07 largely plagiarized by %khc

Notes 07 largely plagiarized by %khc Notes 07 largely plagiarized by %khc Warning This set of notes covers the Fourier transform. However, i probably won t talk about everything here in section; instead i will highlight important properties

More information

6.003 Homework #10 Solutions

6.003 Homework #10 Solutions 6.3 Homework # Solutions Problems. DT Fourier Series Determine the Fourier Series coefficients for each of the following DT signals, which are periodic in N = 8. x [n] / n x [n] n x 3 [n] n x 4 [n] / n

More information

The Discrete-time Fourier Transform

The Discrete-time Fourier Transform The Discrete-time Fourier Transform Rui Wang, Assistant professor Dept. of Information and Communication Tongji University it Email: ruiwang@tongji.edu.cn Outline Representation of Aperiodic signals: The

More information

Complex symmetry Signals and Systems Fall 2015

Complex symmetry Signals and Systems Fall 2015 18-90 Signals and Systems Fall 015 Complex symmetry 1. Complex symmetry This section deals with the complex symmetry property. As an example I will use the DTFT for a aperiodic discrete-time signal. The

More information

Fourier Transform for Continuous Functions

Fourier Transform for Continuous Functions Fourier Transform for Continuous Functions Central goal: representing a signal by a set of orthogonal bases that are corresponding to frequencies or spectrum. Fourier series allows to find the spectrum

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

University Question Paper Solution

University Question Paper Solution Unit 1: Introduction University Question Paper Solution 1. Determine whether the following systems are: i) Memoryless, ii) Stable iii) Causal iv) Linear and v) Time-invariant. i) y(n)= nx(n) ii) y(t)=

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

ELEG 3124 SYSTEMS AND SIGNALS Ch. 5 Fourier Transform

ELEG 3124 SYSTEMS AND SIGNALS Ch. 5 Fourier Transform Department of Electrical Engineering University of Arkansas ELEG 3124 SYSTEMS AND SIGNALS Ch. 5 Fourier Transform Dr. Jingxian Wu wuj@uark.edu OUTLINE 2 Introduction Fourier Transform Properties of Fourier

More information

EE301 Signals and Systems Spring 2016 Exam 2 Thursday, Mar. 31, Cover Sheet

EE301 Signals and Systems Spring 2016 Exam 2 Thursday, Mar. 31, Cover Sheet EE301 Signals and Systems Spring 2016 Exam 2 Thursday, Mar. 31, 2016 Cover Sheet Test Duration: 75 minutes. Coverage: Chapter 4, Hmwks 6-7 Open Book but Closed Notes. One 8.5 in. x 11 in. crib sheet Calculators

More information

Continuous Time Signal Analysis: the Fourier Transform. Lathi Chapter 4

Continuous Time Signal Analysis: the Fourier Transform. Lathi Chapter 4 Continuous Time Signal Analysis: the Fourier Transform Lathi Chapter 4 Topics Aperiodic signal representation by the Fourier integral (CTFT) Continuous-time Fourier transform Transforms of some useful

More information

ENSC327 Communications Systems 2: Fourier Representations. Jie Liang School of Engineering Science Simon Fraser University

ENSC327 Communications Systems 2: Fourier Representations. Jie Liang School of Engineering Science Simon Fraser University ENSC327 Communications Systems 2: Fourier Representations Jie Liang School of Engineering Science Simon Fraser University 1 Outline Chap 2.1 2.5: Signal Classifications Fourier Transform Dirac Delta Function

More information

E2.5 Signals & Linear Systems. Tutorial Sheet 1 Introduction to Signals & Systems (Lectures 1 & 2)

E2.5 Signals & Linear Systems. Tutorial Sheet 1 Introduction to Signals & Systems (Lectures 1 & 2) E.5 Signals & Linear Systems Tutorial Sheet 1 Introduction to Signals & Systems (Lectures 1 & ) 1. Sketch each of the following continuous-time signals, specify if the signal is periodic/non-periodic,

More information

4 The Continuous Time Fourier Transform

4 The Continuous Time Fourier Transform 96 4 The Continuous Time ourier Transform ourier (or frequency domain) analysis turns out to be a tool of even greater usefulness Extension of ourier series representation to aperiodic signals oundation

More information

Signals and Systems Spring 2004 Lecture #9

Signals and Systems Spring 2004 Lecture #9 Signals and Systems Spring 2004 Lecture #9 (3/4/04). The convolution Property of the CTFT 2. Frequency Response and LTI Systems Revisited 3. Multiplication Property and Parseval s Relation 4. The DT Fourier

More information

Chapter 8 The Discrete Fourier Transform

Chapter 8 The Discrete Fourier Transform Chapter 8 The Discrete Fourier Transform Introduction Representation of periodic sequences: the discrete Fourier series Properties of the DFS The Fourier transform of periodic signals Sampling the Fourier

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

06EC44-Signals and System Chapter Fourier Representation for four Signal Classes

06EC44-Signals and System Chapter Fourier Representation for four Signal Classes Chapter 5.1 Fourier Representation for four Signal Classes 5.1.1Mathematical Development of Fourier Transform If the period is stretched without limit, the periodic signal no longer remains periodic but

More information

Linear Filters and Convolution. Ahmed Ashraf

Linear Filters and Convolution. Ahmed Ashraf Linear Filters and Convolution Ahmed Ashraf Linear Time(Shift) Invariant (LTI) Systems The Linear Filters that we are studying in the course belong to a class of systems known as Linear Time Invariant

More information

Chapter 3 Convolution Representation

Chapter 3 Convolution Representation Chapter 3 Convolution Representation DT Unit-Impulse Response Consider the DT SISO system: xn [ ] System yn [ ] xn [ ] = δ[ n] If the input signal is and the system has no energy at n = 0, the output yn

More information

Chapter 3 Fourier Representations of Signals and Linear Time-Invariant Systems

Chapter 3 Fourier Representations of Signals and Linear Time-Invariant Systems Chapter 3 Fourier Representations of Signals and Linear Time-Invariant Systems Introduction Complex Sinusoids and Frequency Response of LTI Systems. Fourier Representations for Four Classes of Signals

More information

New Mexico State University Klipsch School of Electrical Engineering EE312 - Signals and Systems I Fall 2015 Final Exam

New Mexico State University Klipsch School of Electrical Engineering EE312 - Signals and Systems I Fall 2015 Final Exam New Mexico State University Klipsch School of Electrical Engineering EE312 - Signals and Systems I Fall 2015 Name: Solve problems 1 3 and two from problems 4 7. Circle below which two of problems 4 7 you

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

3.2 Complex Sinusoids and Frequency Response of LTI Systems

3.2 Complex Sinusoids and Frequency Response of LTI Systems 3. Introduction. A signal can be represented as a weighted superposition of complex sinusoids. x(t) or x[n]. LTI system: LTI System Output = A weighted superposition of the system response to each complex

More information

Introduction to DFT. Deployment of Telecommunication Infrastructures. Azadeh Faridi DTIC UPF, Spring 2009

Introduction to DFT. Deployment of Telecommunication Infrastructures. Azadeh Faridi DTIC UPF, Spring 2009 Introduction to DFT Deployment of Telecommunication Infrastructures Azadeh Faridi DTIC UPF, Spring 2009 1 Review of Fourier Transform Many signals can be represented by a fourier integral of the following

More information

ENSC327 Communications Systems 2: Fourier Representations. School of Engineering Science Simon Fraser University

ENSC327 Communications Systems 2: Fourier Representations. School of Engineering Science Simon Fraser University ENSC37 Communications Systems : Fourier Representations School o Engineering Science Simon Fraser University Outline Chap..5: Signal Classiications Fourier Transorm Dirac Delta Function Unit Impulse Fourier

More information

Laplace Transforms and use in Automatic Control

Laplace Transforms and use in Automatic Control Laplace Transforms and use in Automatic Control P.S. Gandhi Mechanical Engineering IIT Bombay Acknowledgements: P.Santosh Krishna, SYSCON Recap Fourier series Fourier transform: aperiodic Convolution integral

More information

QUESTION BANK SIGNALS AND SYSTEMS (4 th SEM ECE)

QUESTION BANK SIGNALS AND SYSTEMS (4 th SEM ECE) QUESTION BANK SIGNALS AND SYSTEMS (4 th SEM ECE) 1. For the signal shown in Fig. 1, find x(2t + 3). i. Fig. 1 2. What is the classification of the systems? 3. What are the Dirichlet s conditions of Fourier

More information

Frequency Response and Continuous-time Fourier Series

Frequency Response and Continuous-time Fourier Series Frequency Response and Continuous-time Fourier Series Recall course objectives Main Course Objective: Fundamentals of systems/signals interaction (we d like to understand how systems transform or affect

More information

Homework 4. May An LTI system has an input, x(t) and output y(t) related through the equation y(t) = t e (t t ) x(t 2)dt

Homework 4. May An LTI system has an input, x(t) and output y(t) related through the equation y(t) = t e (t t ) x(t 2)dt Homework 4 May 2017 1. An LTI system has an input, x(t) and output y(t) related through the equation y(t) = t e (t t ) x(t 2)dt Determine the impulse response of the system. Rewriting as y(t) = t e (t

More information

PART 1. Review of DSP. f (t)e iωt dt. F(ω) = f (t) = 1 2π. F(ω)e iωt dω. f (t) F (ω) The Fourier Transform. Fourier Transform.

PART 1. Review of DSP. f (t)e iωt dt. F(ω) = f (t) = 1 2π. F(ω)e iωt dω. f (t) F (ω) The Fourier Transform. Fourier Transform. PART 1 Review of DSP Mauricio Sacchi University of Alberta, Edmonton, AB, Canada The Fourier Transform F() = f (t) = 1 2π f (t)e it dt F()e it d Fourier Transform Inverse Transform f (t) F () Part 1 Review

More information

ESS Finite Impulse Response Filters and the Z-transform

ESS Finite Impulse Response Filters and the Z-transform 9. Finite Impulse Response Filters and the Z-transform We are going to have two lectures on filters you can find much more material in Bob Crosson s notes. In the first lecture we will focus on some of

More information

Properties of LTI Systems

Properties of LTI Systems Properties of LTI Systems Properties of Continuous Time LTI Systems Systems with or without memory: A system is memory less if its output at any time depends only on the value of the input at that same

More information

2.1 Basic Concepts Basic operations on signals Classication of signals

2.1 Basic Concepts Basic operations on signals Classication of signals Haberle³me Sistemlerine Giri³ (ELE 361) 9 Eylül 2017 TOBB Ekonomi ve Teknoloji Üniversitesi, Güz 2017-18 Dr. A. Melda Yüksel Turgut & Tolga Girici Lecture Notes Chapter 2 Signals and Linear Systems 2.1

More information

Representing a Signal

Representing a Signal The Fourier Series Representing a Signal The convolution method for finding the response of a system to an excitation takes advantage of the linearity and timeinvariance of the system and represents the

More information

ELEG3503 Introduction to Digital Signal Processing

ELEG3503 Introduction to Digital Signal Processing ELEG3503 Itroductio to Digital Sigal Processig 1 Itroductio 2 Basics of Sigals ad Systems 3 Fourier aalysis 4 Samplig 5 Liear time-ivariat (LTI) systems 6 z-trasform 7 System Aalysis 8 System Realizatio

More information

Fourier transform representation of CT aperiodic signals Section 4.1

Fourier transform representation of CT aperiodic signals Section 4.1 Fourier transform representation of CT aperiodic signals Section 4. A large class of aperiodic CT signals can be represented by the CT Fourier transform (CTFT). The (CT) Fourier transform (or spectrum)

More information

Review: Continuous Fourier Transform

Review: Continuous Fourier Transform Review: Continuous Fourier Transform Review: convolution x t h t = x τ h(t τ)dτ Convolution in time domain Derivation Convolution Property Interchange the order of integrals Let Convolution Property By

More information

Fourier Analysis Overview (0B)

Fourier Analysis Overview (0B) CTFS: Continuous Time Fourier Series CTFT: Continuous Time Fourier Transform DTFS: Fourier Series DTFT: Fourier Transform DFT: Discrete Fourier Transform Copyright (c) 2009-2016 Young W. Lim. Permission

More information

Review of Fourier Transform

Review of Fourier Transform Review of Fourier Transform Fourier series works for periodic signals only. What s about aperiodic signals? This is very large & important class of signals Aperiodic signal can be considered as periodic

More information

Lecture 27 Frequency Response 2

Lecture 27 Frequency Response 2 Lecture 27 Frequency Response 2 Fundamentals of Digital Signal Processing Spring, 2012 Wei-Ta Chu 2012/6/12 1 Application of Ideal Filters Suppose we can generate a square wave with a fundamental period

More information

2.161 Signal Processing: Continuous and Discrete

2.161 Signal Processing: Continuous and Discrete MI OpenCourseWare http://ocw.mit.edu.6 Signal Processing: Continuous and Discrete Fall 8 For information about citing these materials or our erms of Use, visit: http://ocw.mit.edu/terms. MASSACHUSES INSIUE

More information

Module 3 : Sampling and Reconstruction Lecture 22 : Sampling and Reconstruction of Band-Limited Signals

Module 3 : Sampling and Reconstruction Lecture 22 : Sampling and Reconstruction of Band-Limited Signals Module 3 : Sampling and Reconstruction Lecture 22 : Sampling and Reconstruction of Band-Limited Signals Objectives Scope of this lecture: If a Continuous Time (C.T.) signal is to be uniquely represented

More information

Topic 3: Fourier Series (FS)

Topic 3: Fourier Series (FS) ELEC264: Signals And Systems Topic 3: Fourier Series (FS) o o o o Introduction to frequency analysis of signals CT FS Fourier series of CT periodic signals Signal Symmetry and CT Fourier Series Properties

More information

Representation of Signals and Systems. Lecturer: David Shiung

Representation of Signals and Systems. Lecturer: David Shiung Representation of Signals and Systems Lecturer: David Shiung 1 Abstract (1/2) Fourier analysis Properties of the Fourier transform Dirac delta function Fourier transform of periodic signals Fourier-transform

More information

Review of Analog Signal Analysis

Review of Analog Signal Analysis Review of Analog Signal Analysis Chapter Intended Learning Outcomes: (i) Review of Fourier series which is used to analyze continuous-time periodic signals (ii) Review of Fourier transform which is used

More information

Question Paper Code : AEC11T02

Question Paper Code : AEC11T02 Hall Ticket No Question Paper Code : AEC11T02 VARDHAMAN COLLEGE OF ENGINEERING (AUTONOMOUS) Affiliated to JNTUH, Hyderabad Four Year B. Tech III Semester Tutorial Question Bank 2013-14 (Regulations: VCE-R11)

More information

Fourier Series Representation of

Fourier Series Representation of Fourier Series Representation of Periodic Signals Rui Wang, Assistant professor Dept. of Information and Communication Tongji University it Email: ruiwang@tongji.edu.cn Outline The response of LIT system

More information

EE 224 Signals and Systems I Review 1/10

EE 224 Signals and Systems I Review 1/10 EE 224 Signals and Systems I Review 1/10 Class Contents Signals and Systems Continuous-Time and Discrete-Time Time-Domain and Frequency Domain (all these dimensions are tightly coupled) SIGNALS SYSTEMS

More information

Signals & Systems. Lecture 5 Continuous-Time Fourier Transform. Alp Ertürk

Signals & Systems. Lecture 5 Continuous-Time Fourier Transform. Alp Ertürk Signals & Systems Lecture 5 Continuous-Time Fourier Transform Alp Ertürk alp.erturk@kocaeli.edu.tr Fourier Series Representation of Continuous-Time Periodic Signals Synthesis equation: x t = a k e jkω

More information

How to manipulate Frequencies in Discrete-time Domain? Two Main Approaches

How to manipulate Frequencies in Discrete-time Domain? Two Main Approaches How to manipulate Frequencies in Discrete-time Domain? Two Main Approaches Difference Equations (an LTI system) x[n]: input, y[n]: output That is, building a system that maes use of the current and previous

More information

6.003: Signals and Systems. CT Fourier Transform

6.003: Signals and Systems. CT Fourier Transform 6.003: Signals and Systems CT Fourier Transform April 8, 200 CT Fourier Transform Representing signals by their frequency content. X(jω)= x(t)e jωt dt ( analysis equation) x(t)= 2π X(jω)e jωt dω ( synthesis

More information

LECTURE 12 Sections Introduction to the Fourier series of periodic signals

LECTURE 12 Sections Introduction to the Fourier series of periodic signals Signals and Systems I Wednesday, February 11, 29 LECURE 12 Sections 3.1-3.3 Introduction to the Fourier series of periodic signals Chapter 3: Fourier Series of periodic signals 3. Introduction 3.1 Historical

More information

Chapter 5 Frequency Domain Analysis of Systems

Chapter 5 Frequency Domain Analysis of Systems Chapter 5 Frequency Domain Analysis of Systems CT, LTI Systems Consider the following CT LTI system: xt () ht () yt () Assumption: the impulse response h(t) is absolutely integrable, i.e., ht ( ) dt< (this

More information

Fourier Series and Fourier Transforms

Fourier Series and Fourier Transforms Fourier Series and Fourier Transforms Houshou Chen Dept. of Electrical Engineering, National Chung Hsing University E-mail: houshou@ee.nchu.edu.tw H.S. Chen Fourier Series and Fourier Transforms 1 Why

More information

Introduction to Linear Time-Invariant Systems

Introduction to Linear Time-Invariant Systems Introduction to Linear Time-Invariant Systems Marco Cagnazzo Multimedia Networking 1 Signal spaces Discrete-time signals (sequences) u: n Z u n C If n N, u n R, then u is referred to as a real sequence

More information

6.003: Signals and Systems. CT Fourier Transform

6.003: Signals and Systems. CT Fourier Transform 6.003: Signals and Systems CT Fourier Transform April 8, 200 CT Fourier Transform Representing signals by their frequency content. X(jω)= x(t)e jωt dt ( analysis equation) x(t)= X(jω)e jωt dω ( synthesis

More information

Chapter 6: Applications of Fourier Representation Houshou Chen

Chapter 6: Applications of Fourier Representation Houshou Chen Chapter 6: Applications of Fourier Representation Houshou Chen Dept. of Electrical Engineering, National Chung Hsing University E-mail: houshou@ee.nchu.edu.tw H.S. Chen Chapter6: Applications of Fourier

More information

Flash File. Module 3 : Sampling and Reconstruction Lecture 28 : Discrete time Fourier transform and its Properties. Objectives: Scope of this Lecture:

Flash File. Module 3 : Sampling and Reconstruction Lecture 28 : Discrete time Fourier transform and its Properties. Objectives: Scope of this Lecture: Module 3 : Sampling and Reconstruction Lecture 28 : Discrete time Fourier transform and its Properties Objectives: Scope of this Lecture: In the previous lecture we defined digital signal processing and

More information

EE 3054: Signals, Systems, and Transforms Summer It is observed of some continuous-time LTI system that the input signal.

EE 3054: Signals, Systems, and Transforms Summer It is observed of some continuous-time LTI system that the input signal. EE 34: Signals, Systems, and Transforms Summer 7 Test No notes, closed book. Show your work. Simplify your answers. 3. It is observed of some continuous-time LTI system that the input signal = 3 u(t) produces

More information

The Johns Hopkins University Department of Electrical and Computer Engineering Introduction to Linear Systems Fall 2002.

The Johns Hopkins University Department of Electrical and Computer Engineering Introduction to Linear Systems Fall 2002. The Johns Hopkins University Department of Electrical and Computer Engineering 505.460 Introduction to Linear Systems Fall 2002 Final exam Name: You are allowed to use: 1. Table 3.1 (page 206) & Table

More information

Interconnection of LTI Systems

Interconnection of LTI Systems EENG226 Signals and Systems Chapter 2 Time-Domain Representations of Linear Time-Invariant Systems Interconnection of LTI Systems Prof. Dr. Hasan AMCA Electrical and Electronic Engineering Department (ee.emu.edu.tr)

More information

Probability and Statistics for Final Year Engineering Students

Probability and Statistics for Final Year Engineering Students Probability and Statistics for Final Year Engineering Students By Yoni Nazarathy, Last Updated: May 24, 2011. Lecture 6p: Spectral Density, Passing Random Processes through LTI Systems, Filtering Terms

More information

Lecture 19 IIR Filters

Lecture 19 IIR Filters Lecture 19 IIR Filters Fundamentals of Digital Signal Processing Spring, 2012 Wei-Ta Chu 2012/5/10 1 General IIR Difference Equation IIR system: infinite-impulse response system The most general class

More information

Chapter 5 Frequency Domain Analysis of Systems

Chapter 5 Frequency Domain Analysis of Systems Chapter 5 Frequency Domain Analysis of Systems CT, LTI Systems Consider the following CT LTI system: xt () ht () yt () Assumption: the impulse response h(t) is absolutely integrable, i.e., ht ( ) dt< (this

More information

20.6. Transfer Functions. Introduction. Prerequisites. Learning Outcomes

20.6. Transfer Functions. Introduction. Prerequisites. Learning Outcomes Transfer Functions 2.6 Introduction In this Section we introduce the concept of a transfer function and then use this to obtain a Laplace transform model of a linear engineering system. (A linear engineering

More information

Chapter 6: The Laplace Transform. Chih-Wei Liu

Chapter 6: The Laplace Transform. Chih-Wei Liu Chapter 6: The Laplace Transform Chih-Wei Liu Outline Introduction The Laplace Transform The Unilateral Laplace Transform Properties of the Unilateral Laplace Transform Inversion of the Unilateral Laplace

More information

Lecture 13: Pole/Zero Diagrams and All Pass Systems

Lecture 13: Pole/Zero Diagrams and All Pass Systems EE518 Digital Signal Processing University of Washington Autumn 2001 Dept. of Electrical Engineering Lecture 13: Pole/Zero Diagrams and All Pass Systems No4, 2001 Prof: J. Bilmes

More information

EA2.3 - Electronics 2 1

EA2.3 - Electronics 2 1 In the previous lecture, I talked about the idea of complex frequency s, where s = σ + jω. Using such concept of complex frequency allows us to analyse signals and systems with better generality. In this

More information

DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING EXAMINATIONS 2010

DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING EXAMINATIONS 2010 [E2.5] IMPERIAL COLLEGE LONDON DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING EXAMINATIONS 2010 EEE/ISE PART II MEng. BEng and ACGI SIGNALS AND LINEAR SYSTEMS Time allowed: 2:00 hours There are FOUR

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

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

ENGIN 211, Engineering Math. Laplace Transforms

ENGIN 211, Engineering Math. Laplace Transforms ENGIN 211, Engineering Math Laplace Transforms 1 Why Laplace Transform? Laplace transform converts a function in the time domain to its frequency domain. It is a powerful, systematic method in solving

More information

Fourier series for continuous and discrete time signals

Fourier series for continuous and discrete time signals 8-9 Signals and Systems Fall 5 Fourier series for continuous and discrete time signals The road to Fourier : Two weeks ago you saw that if we give a complex exponential as an input to a system, the output

More information

LOPE3202: Communication Systems 10/18/2017 2

LOPE3202: Communication Systems 10/18/2017 2 By Lecturer Ahmed Wael Academic Year 2017-2018 LOPE3202: Communication Systems 10/18/2017 We need tools to build any communication system. Mathematics is our premium tool to do work with signals and systems.

More information

Course roadmap. ME451: Control Systems. Example of Laplace transform. Lecture 2 Laplace transform. Laplace transform

Course roadmap. ME451: Control Systems. Example of Laplace transform. Lecture 2 Laplace transform. Laplace transform ME45: Control Systems Lecture 2 Prof. Jongeun Choi Department of Mechanical Engineering Michigan State University Modeling Transfer function Models for systems electrical mechanical electromechanical Block

More information

2.161 Signal Processing: Continuous and Discrete Fall 2008

2.161 Signal Processing: Continuous and Discrete Fall 2008 MIT OpenCourseWare http://ocw.mit.edu 2.161 Signal Processing: Continuous and Discrete Fall 2008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. Massachusetts

More information

Lecture 1 From Continuous-Time to Discrete-Time

Lecture 1 From Continuous-Time to Discrete-Time Lecture From Continuous-Time to Discrete-Time Outline. Continuous and Discrete-Time Signals and Systems................. What is a signal?................................2 What is a system?.............................

More information

Introduction & Laplace Transforms Lectures 1 & 2

Introduction & Laplace Transforms Lectures 1 & 2 Introduction & Lectures 1 & 2, Professor Department of Electrical and Computer Engineering Colorado State University Fall 2016 Control System Definition of a Control System Group of components that collectively

More information

信號與系統 Signals and Systems

信號與系統 Signals and Systems Spring 2013 Flowchart Introduction (Chap 1) LTI & Convolution (Chap 2) NTUEE-SS10-Z-2 信號與系統 Signals and Systems Chapter SS-10 The z-transform FS (Chap 3) Periodic Bounded/Convergent CT DT FT Aperiodic

More information

Math Homework 3 Solutions. (1 y sin x) dx + (cos x) dy = 0. = sin x =

Math Homework 3 Solutions. (1 y sin x) dx + (cos x) dy = 0. = sin x = 2.6 #10: Determine if the equation is exact. If so, solve it. Math 315-01 Homework 3 Solutions (1 y sin x) dx + (cos x) dy = 0 Solution: Let P (x, y) = 1 y sin x and Q(x, y) = cos x. Note P = sin x = Q

More information

The formulas for derivatives are particularly useful because they reduce ODEs to algebraic expressions. Consider the following ODE d 2 dx + p d

The formulas for derivatives are particularly useful because they reduce ODEs to algebraic expressions. Consider the following ODE d 2 dx + p d Solving ODEs using Fourier Transforms The formulas for derivatives are particularly useful because they reduce ODEs to algebraic expressions. Consider the following ODE d 2 dx + p d 2 dx + q f (x) R(x)

More information

Representation of Signals & Systems

Representation of Signals & Systems Representation of Signals & Systems Reference: Chapter 2,Communication Systems, Simon Haykin. Hilbert Transform Fourier transform frequency content of a signal (frequency selectivity designing frequency-selective

More information

Introduction ODEs and Linear Systems

Introduction ODEs and Linear Systems BENG 221 Mathematical Methods in Bioengineering ODEs and Linear Systems Gert Cauwenberghs Department of Bioengineering UC San Diego 1.1 Course Objectives 1. Acquire methods for quantitative analysis and

More information

Stochastic Processes

Stochastic Processes Elements of Lecture II Hamid R. Rabiee with thanks to Ali Jalali Overview Reading Assignment Chapter 9 of textbook Further Resources MIT Open Course Ware S. Karlin and H. M. Taylor, A First Course in Stochastic

More information

II/IV B.Tech (Regular/Supplementary) DEGREE EXAMINATION. Answer ONE question from each unit.

II/IV B.Tech (Regular/Supplementary) DEGREE EXAMINATION. Answer ONE question from each unit. 14ECEI302/EC 212 1. Answer all questions (1X12=12 Marks) a What are the applications of linked list? b Compare singly linked list and doubly linked list. c Define ADT. d What are the basic operations of

More information

Control Systems. Laplace domain analysis

Control Systems. Laplace domain analysis Control Systems Laplace domain analysis L. Lanari outline introduce the Laplace unilateral transform define its properties show its advantages in turning ODEs to algebraic equations define an Input/Output

More information

ECE 301: Signals and Systems Homework Assignment #5

ECE 301: Signals and Systems Homework Assignment #5 ECE 30: Signals and Systems Homework Assignment #5 Due on November, 205 Professor: Aly El Gamal TA: Xianglun Mao Aly El Gamal ECE 30: Signals and Systems Homework Assignment #5 Problem Problem Compute

More information

ECG782: Multidimensional Digital Signal Processing

ECG782: Multidimensional Digital Signal Processing Professor Brendan Morris, SEB 3216, brendan.morris@unlv.edu ECG782: Multidimensional Digital Signal Processing Filtering in the Frequency Domain http://www.ee.unlv.edu/~b1morris/ecg782/ 2 Outline Background

More information

E : Lecture 1 Introduction

E : Lecture 1 Introduction E85.2607: Lecture 1 Introduction 1 Administrivia 2 DSP review 3 Fun with Matlab E85.2607: Lecture 1 Introduction 2010-01-21 1 / 24 Course overview Advanced Digital Signal Theory Design, analysis, and implementation

More information

This homework will not be collected or graded. It is intended to help you practice for the final exam. Solutions will be posted.

This homework will not be collected or graded. It is intended to help you practice for the final exam. Solutions will be posted. 6.003 Homework #14 This homework will not be collected or graded. It is intended to help you practice for the final exam. Solutions will be posted. Problems 1. Neural signals The following figure illustrates

More information

University of Kentucky Department of Electrical and Computer Engineering. EE421G: Signals and Systems I Fall 2007

University of Kentucky Department of Electrical and Computer Engineering. EE421G: Signals and Systems I Fall 2007 University of Kentucky Department of Electrical an Computer Engineering EE4G: Signals an Systems I Fall 7 Issue: October 4, 7 Problem Set 6 Due: October, 7 (In class) Reaing Assignments: Rea Chapter 3.7,

More information

( ) f (k) = FT (R(x)) = R(k)

( ) f (k) = FT (R(x)) = R(k) Solving ODEs using Fourier Transforms The formulas for derivatives are particularly useful because they reduce ODEs to algebraic expressions. Consider the following ODE d 2 dx + p d 2 dx + q f (x) = R(x)

More information

Module 4. Related web links and videos. 1. FT and ZT

Module 4. Related web links and videos. 1.  FT and ZT Module 4 Laplace transforms, ROC, rational systems, Z transform, properties of LT and ZT, rational functions, system properties from ROC, inverse transforms Related web links and videos Sl no Web link

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