Lecture 4&5 MATLAB applications In Signal Processing. Dr. Bedir Yousif

Size: px
Start display at page:

Download "Lecture 4&5 MATLAB applications In Signal Processing. Dr. Bedir Yousif"

Transcription

1 Lecture 4&5 MATLAB applications In Signal Processing Dr. Bedir Yousif

2 Signal Analysis Fourier Series and Fourier Transform Trigonometric Fourier Series Where w0=2*pi/tp and the Fourier coefficients a n and b n are determined by the following equations

3 Fourier Series Another Form of trigonometric Fourier Series a 0 /2 is the dc component of the series and is the average value of g(t) over a period. The total power in g(t) is given by the Parseval s equation: And

4 Fourier Series Example 1: Using Fourier series expansion, a square wave with a period of 2 ms, peak-to peak value of 2 volts and average value of zero volt can be expressed as Where f 0 = 500 Hz if a(t) is given as Write a MATLAB program to plot a(t) from 0 to 4 ms at intervals of 0.05 ms and to show that a(t) is a good approximation of g(t).

5 Fourier Series Solution clear all f = 500; c = 4/pi; w0 = 2*pi*f; t=0:0.05e-3:4e-3; s=zeros(1,length(t)); for n = 1: 12 s = s+c*(1/(2*n - 1))*sin((2*n - 1)*w0*t); end plot(t,s) xlabel('time, s') ylabel('amplitude, V') title('fourier series expansion')

6 Fourier Series Solution

7 Fourier Series Solution

8 Exponential Fourier Series Fourier Series The coefficient c n is related to the coefficients a n and b n In addition, cn relates to A n and φ n of Equations

9 Fourier Series The plot of c n versus frequency is termed the discrete amplitude spectrum or the line spectrum. A similar plot of cn versus frequency is called the discrete phase spectrum If an input signal x n (t) passes through a system with transfer function H(w), then the output of the system y n (t) is

10 Fourier Series If an input signal x n (t) written in complex F.S the response at the output of the system is

11 Fourier Series Example 2 For the full-wave rectifier waveform shown in Figure, the period is 1/60 s and the amplitude is Volts. (a) Write a MATLAB program to obtain the exponential (b) Fourier series coefficients cn for n = 0,1, 2,.., 19 (b) Find the dc value. (c) Plot the amplitude and phase spectrum.

12 Fourier Series Solution % generate the full-wave rectifier waveform f1 = 60; inv = 1/f1; inc = 1/(80*f1); tnum = 3*inv; t = 0:inc:tnum; g1 = 120*sqrt(2)*sin(2*pi*f1*t); g = abs(g1); N = length(g); % obtain the exponential Fourier series coefficients num = 20; for i = 1:num for m = 1:N cint(m) = exp(-j*2*pi*(i-1)*m/n)*g(m);

13 Fourier Series Solution end c(i) = sum(cint)/n; end cmag = abs(c); cphase = angle(c); %print dc value disp('dc value of g(t)'); cmag(1)% c0 % plot the magnitude and phase spectrum f = (0:num-1)*60; subplot(121), stem(f(1:5),cmag(1:5)) title('amplitude spectrum') xlabel('frequency, Hz') subplot(122), stem(f(1:5),cphase(1:5)) title('phase spectrum') xlabel('frequency, Hz')

14 Result Fourier Series Spectrum

15 Result Fourier Series dc value of g(t) ans =

16 Fourier Series Example.3 The periodic signal shown in Figure (i) Show that its exponential Fourier series expansion can be expressed as (ii) Using a MATLAB program, synthesize g(t) using 20 terms, i.

17 Solution Fourier Series

18 Fourier Series Solution % synthesis of g(t) using exponential Fourier series expansion dt = 0.05; tpts = 8.0/dt +1;% No. of points on time axis cst = exp(2) - exp(-2); for n = -10:10 for m = 1:tpts g1(n+11,m) = ((0.5*cst*((-1)^n))/(2+j*n*pi))*(exp(j*n*pi*dt*(m-1))); end end for m = 1: tpts g2 = g1(:,m); g3(m) = sum(g2); end g = g3'; t = -4:0.05:4.0; plot(t,g) xlabel('time, s') ylabel('amplitude'); title('approximation of g(t)')

19 Solution Fourier Series Approximation of g(t).

20 Fourier Series Fourier Series for Several Periodic Signals

21 Fourier Transform formula: Fourier transform Inverse Fourier Transform formula: If g(t) is continuous and nonperiodic, then G(f) will be continuous and periodic. However, if g(t) is continuous and periodic, then G(f) will discrete and nonperiodic; that is

22 Fourier transform Complex exponential Fourier coefficient: Properties of Fourier transform 1- Linearity Ag 1 (t) +bg 2 (t) ag 1 (f) + bg 2 (f) Where a and b are constants 2- Time scaling

23 Properties of Fourier transform 3- Duality G(t) g( f ) 4- Time shifting g(t t ) G( f ) exp( j2π ft ) 5- Frequency Shifting exp(j2 f c t)g(t) G(f -f c ) 6- Differentiation in the time domain

24 Properties of Fourier transform 7- Integration in the time domain 8- Multiplication in the time domain 9- Convolution in the time domain

25 Properties of Fourier transform 7- Integration in the time domain 8- Multiplication in the time domain 9- Convolution in the time domain

26 Thanks

CEMTool Tutorial. Fourier Analysis

CEMTool Tutorial. Fourier Analysis CEMTool Tutorial Fourier Aalysis Overview This tutorial is part of the CEMWARE series. Each tutorial i this series will teach you a specific topic of commo applicatios by explaiig theoretical cocepts ad

More information

Fourier Series and Transform KEEE343 Communication Theory Lecture #7, March 24, Prof. Young-Chai Ko

Fourier Series and Transform KEEE343 Communication Theory Lecture #7, March 24, Prof. Young-Chai Ko Fourier Series and Transform KEEE343 Communication Theory Lecture #7, March 24, 20 Prof. Young-Chai Ko koyc@korea.ac.kr Summary Fourier transform Properties Fourier transform of special function Fourier

More information

Correlation, discrete Fourier transforms and the power spectral density

Correlation, discrete Fourier transforms and the power spectral density Correlation, discrete Fourier transforms and the power spectral density visuals to accompany lectures, notes and m-files by Tak Igusa tigusa@jhu.edu Department of Civil Engineering Johns Hopkins University

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

Solutions to Assignment 4

Solutions to Assignment 4 EE35 Spectrum Analysis and Discrete Time Systems (Fall 5) Solutions to Assignment. Consider the continuous-time periodic signal: x(t) = sin(t 3) + sin(6t) (8) [] (a) Obviously, the fundamental frequency

More information

ANSWERS TO SELECTED EXCERCISES, CH 6-7

ANSWERS TO SELECTED EXCERCISES, CH 6-7 Exercise 6.2 a. We start from equation (6.4) and plug in δ(t) for f(t) F(jω) = δ(t)e jωt dt By the sifting property of δ(t), we see that F(jω) = e jω0 = 1 b. Starting from equation (6.8) and plugging in

More information

2 Background: Fourier Series Analysis and Synthesis

2 Background: Fourier Series Analysis and Synthesis Signal Processing First Lab 15: Fourier Series Pre-Lab and Warm-Up: You should read at least the Pre-Lab and Warm-up sections of this lab assignment and go over all exercises in the Pre-Lab section before

More information

(i) Represent continuous-time periodic signals using Fourier series

(i) Represent continuous-time periodic signals using Fourier series Fourier Series Chapter Intended Learning Outcomes: (i) Represent continuous-time periodic signals using Fourier series (ii) (iii) Understand the properties of Fourier series Understand the relationship

More information

ω 0 = 2π/T 0 is called the fundamental angular frequency and ω 2 = 2ω 0 is called the

ω 0 = 2π/T 0 is called the fundamental angular frequency and ω 2 = 2ω 0 is called the he ime-frequency Concept []. Review of Fourier Series Consider the following set of time functions {3A sin t, A sin t}. We can represent these functions in different ways by plotting the amplitude versus

More information

Solutions to Problems in Chapter 4

Solutions to Problems in Chapter 4 Solutions to Problems in Chapter 4 Problems with Solutions Problem 4. Fourier Series of the Output Voltage of an Ideal Full-Wave Diode Bridge Rectifier he nonlinear circuit in Figure 4. is a full-wave

More information

Signals & Systems. Lecture 4 Fourier Series Properties & Discrete-Time Fourier Series. Alp Ertürk

Signals & Systems. Lecture 4 Fourier Series Properties & Discrete-Time Fourier Series. Alp Ertürk Signals & Systems Lecture 4 Fourier Series Properties & Discrete-Time Fourier Series Alp Ertürk alp.erturk@kocaeli.edu.tr Fourier Series Representation of Continuous-Time Periodic Signals Synthesis equation:

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

EE3210 Lab 3: Periodic Signal Representation by Fourier Series

EE3210 Lab 3: Periodic Signal Representation by Fourier Series City University of Hong Kong Department of Electronic Engineering EE321 Lab 3: Periodic Signal Representation by Fourier Series Prelab: Read the Background section. Complete Section 2.2(b), which asks

More information

Fourier series: Additional notes

Fourier series: Additional notes Fourier series: Additional notes Linking Fourier series representations for signals Rectangular waveform Require FS expansion of signal y(t) below: 1 y(t) 1 4 4 8 12 t (seconds) Period T = 8, so ω = 2π/T

More information

EP375 Computational Physics

EP375 Computational Physics EP375 Computational Physics opic 11 FOURIER RANSFORM Department of Engineering Physics University of Gaziantep Apr 2014 Sayfa 1 Content 1. Introduction 2. Continues Fourier rans. 3. DF in MALAB and C++

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

function [freq,coeff,apspec] = fourier_coeff(fun,t0,t,m,n,method,res,num_p)

function [freq,coeff,apspec] = fourier_coeff(fun,t0,t,m,n,method,res,num_p) function [freq,coeff,apspec] = fourier_coeff(fun,t0,t,m,n,method,res,num_p) Calculate the Fourier coefficients of the series expansion of a function, and the amplitude and phase spectra. The script contains

More information

EE 313 Linear Systems and Signals The University of Texas at Austin. Solution Set for Homework #1 on Sinusoidal Signals

EE 313 Linear Systems and Signals The University of Texas at Austin. Solution Set for Homework #1 on Sinusoidal Signals Solution Set for Homework #1 on Sinusoidal Signals By Mr. Houshang Salimian and Prof. Brian L. Evans September 7, 2018 1. Prologue: This problem helps you to identify the points of interest in a sinusoidal

More information

CHAPTER 4 FOURIER SERIES S A B A R I N A I S M A I L

CHAPTER 4 FOURIER SERIES S A B A R I N A I S M A I L CHAPTER 4 FOURIER SERIES 1 S A B A R I N A I S M A I L Outline Introduction of the Fourier series. The properties of the Fourier series. Symmetry consideration Application of the Fourier series to circuit

More information

CE 513: STATISTICAL METHODS

CE 513: STATISTICAL METHODS 28-8-217/CE 68 CE 513: STATISTICAL METHODS IN CIVIL ENGINEERING Lecture: Introduction to Fourier transforms Dr. Budhaditya Hazra Room: N-37 Department of Civil Engineering 1 Fourier Analysis Fourier Series

More information

ELEC 202 Electric Circuit Analysis II Lecture 10(a) Complex Arithmetic and Rectangular/Polar Forms

ELEC 202 Electric Circuit Analysis II Lecture 10(a) Complex Arithmetic and Rectangular/Polar Forms Dr. Gregory J. Mazzaro Spring 2016 ELEC 202 Electric Circuit Analysis II Lecture 10(a) Complex Arithmetic and Rectangular/Polar Forms THE CITADEL, THE MILITARY COLLEGE OF SOUTH CAROLINA 171 Moultrie Street,

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

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

EE 311 February 22, 2019 Lecture 13

EE 311 February 22, 2019 Lecture 13 EE 311 February, 019 Lecture 13 Minimum Phase FIR filters Geometric Interpretation of P/Z locations Minimum Phase System - A system is said to be a minimum phase system if the deviation from zero in the

More information

SYLLABUS. osmania university CHAPTER - 1 : TRANSIENT RESPONSE CHAPTER - 2 : LAPLACE TRANSFORM OF SIGNALS

SYLLABUS. osmania university CHAPTER - 1 : TRANSIENT RESPONSE CHAPTER - 2 : LAPLACE TRANSFORM OF SIGNALS i SYLLABUS osmania university UNIT - I CHAPTER - 1 : TRANSIENT RESPONSE Initial Conditions in Zero-Input Response of RC, RL and RLC Networks, Definitions of Unit Impulse, Unit Step and Ramp Functions,

More information

Fourier analysis of discrete-time signals. (Lathi Chapt. 10 and these slides)

Fourier analysis of discrete-time signals. (Lathi Chapt. 10 and these slides) Fourier analysis of discrete-time signals (Lathi Chapt. 10 and these slides) Towards the discrete-time Fourier transform How we will get there? Periodic discrete-time signal representation by Discrete-time

More information

Fourier Transform. Find the Fourier series for a periodic waveform Determine the output of a filter when the input is a periodic function

Fourier Transform. Find the Fourier series for a periodic waveform Determine the output of a filter when the input is a periodic function Objectives: Be able to Fourier Transform Find the Fourier series for a periodic waveform Determine the output of a filter when the input is a periodic function Filters with a Single Sinusoidal Input: Suppose

More information

FFT, total energy, and energy spectral density computations in MATLAB Aaron Scher

FFT, total energy, and energy spectral density computations in MATLAB Aaron Scher FFT, total energy, and energy spectral density computations in MATLAB Aaron Scher Everything presented here is specifically focused on non-periodic signals with finite energy (also called energy signals

More information

The Continuous Time Fourier Transform

The Continuous Time Fourier Transform COMM 401: Signals & Systems Theory Lecture 8 The Continuous Time Fourier Transform Fourier Transform Continuous time CT signals Discrete time DT signals Aperiodic signals nonperiodic periodic signals Aperiodic

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

FFT Octave Codes (1B) Young Won Lim 7/6/17

FFT Octave Codes (1B) Young Won Lim 7/6/17 FFT Octave Codes (1B) Copyright (c) 2009-2017 Young W. Lim. Permission is granted to copy, distribute and/or modify this document under the terms of the GNU Free Documentation License, Version 1.2 or any

More information

Central to this is two linear transformations: the Fourier Transform and the Laplace Transform. Both will be considered in later lectures.

Central to this is two linear transformations: the Fourier Transform and the Laplace Transform. Both will be considered in later lectures. In this second lecture, I will be considering signals from the frequency perspective. This is a complementary view of signals, that in the frequency domain, and is fundamental to the subject of signal

More information

Chapter 4 The Fourier Series and Fourier Transform

Chapter 4 The Fourier Series and Fourier Transform Chapter 4 The Fourier Series and Fourier Transform Representation of Signals in Terms of Frequency Components Consider the CT signal defined by N xt () = Acos( ω t+ θ ), t k = 1 k k k The frequencies `present

More information

Chapter 4 The Fourier Series and Fourier Transform

Chapter 4 The Fourier Series and Fourier Transform Chapter 4 The Fourier Series and Fourier Transform Fourier Series Representation of Periodic Signals Let x(t) be a CT periodic signal with period T, i.e., xt ( + T) = xt ( ), t R Example: the rectangular

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

LAB # 5 HANDOUT. »»» The N-point DFT is converted into two DFTs each of N/2 points. N = -W N Then, the following formulas must be used. = k=0,...

LAB # 5 HANDOUT. »»» The N-point DFT is converted into two DFTs each of N/2 points. N = -W N Then, the following formulas must be used. = k=0,... EEE4 Lab Handout. FAST FOURIER TRANSFORM LAB # 5 HANDOUT Data Sequence A = x, x, x, x3, x4, x5, x6, x7»»» The N-point DFT is converted into two DFTs each of N/ points. x, x, x4, x6 x, x3, x5, x7»»» N =e

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

A3. Frequency Representation of Continuous Time and Discrete Time Signals

A3. Frequency Representation of Continuous Time and Discrete Time Signals A3. Frequency Representation of Continuous Time and Discrete Time Signals Objectives Define the magnitude and phase plots of continuous time sinusoidal signals Extend the magnitude and phase plots to discrete

More information

GEORGIA INSTITUTE OF TECHNOLOGY SCHOOL OF ELECTRICAL AND COMPUTER ENGINEERING

GEORGIA INSTITUTE OF TECHNOLOGY SCHOOL OF ELECTRICAL AND COMPUTER ENGINEERING GEORGIA INSTITUTE OF TECHNOLOGY SCHOOL OF ELECTRICAL AND COMUTER ENGINEERING ECE 2026 Summer 208 roblem Set #3 Assigned: May 27, 208 Due: June 5, 208 Reading: Chapter 3 on Spectrum Representation, and

More information

Solutions - Homework # 3

Solutions - Homework # 3 ECE-34: Signals and Systems Summer 23 PROBLEM One period of the DTFS coefficients is given by: X[] = (/3) 2, 8. Solutions - Homewor # 3 a) What is the fundamental period 'N' of the time-domain signal x[n]?

More information

Section Kamen and Heck And Harman. Fourier Transform

Section Kamen and Heck And Harman. Fourier Transform s Section 3.4-3.7 Kamen and Heck And Harman 1 3.4 Definition (Equation 3.30) Exists if integral converges (Equation 3.31) Example 3.7 Constant Signal Does not have a Fourier transform in the ordinary sense.

More information

Review of DC Electric Circuit. DC Electric Circuits Examples (source:

Review of DC Electric Circuit. DC Electric Circuits Examples (source: Review of DC Electric Circuit DC Electric Circuits Examples (source: http://hyperphysics.phyastr.gsu.edu/hbase/electric/dcex.html) 1 Review - DC Electric Circuit Multisim Circuit Simulation DC Circuit

More information

( 1) EE 313 Linear Signals & Systems (Fall 2018) Solution Set for Homework #10 on Laplace Transforms

( 1) EE 313 Linear Signals & Systems (Fall 2018) Solution Set for Homework #10 on Laplace Transforms EE 33 Linear Signal & Sytem (Fall 08) Solution Set for Homework #0 on Laplace Tranform By: Mr. Houhang Salimian & Prof. Brian L. Evan Problem. a) xt () = ut () ut ( ) From lecture Lut { ()} = and { } t

More information

The result can also be expressed in the alternate form of Eq by computing the amplitude and the phase shift,

The result can also be expressed in the alternate form of Eq by computing the amplitude and the phase shift, CHAPER 6 6. he angular frequency can be computed as = /4 =.6799. he various summations required for the normal equations can be set up as t y cos( t) sin( t) sin( t)cos( t) cos ( t) sin ( t) ycos( t) ysin(

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

I. Signals & Sinusoids

I. Signals & Sinusoids I. Signals & Sinusoids [p. 3] Signal definition Sinusoidal signal Plotting a sinusoid [p. 12] Signal operations Time shifting Time scaling Time reversal Combining time shifting & scaling [p. 17] Trigonometric

More information

Basics about Fourier analysis

Basics about Fourier analysis Jérôme Gilles UCLA PART ONE Fourier analysis On the menu... Introduction - some history... Notations. Fourier series. Continuous Fourier transform. Discrete Fourier transform. Properties. 2D extension.

More information

IB Paper 6: Signal and Data Analysis

IB Paper 6: Signal and Data Analysis IB Paper 6: Signal and Data Analysis Handout 2: Fourier Series S Godsill Signal Processing and Communications Group, Engineering Department, Cambridge, UK Lent 2015 1 / 1 Fourier Series Revision of Basics

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

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

Communication Signals (Haykin Sec. 2.4 and Ziemer Sec Sec. 2.4) KECE321 Communication Systems I

Communication Signals (Haykin Sec. 2.4 and Ziemer Sec Sec. 2.4) KECE321 Communication Systems I Communication Signals (Haykin Sec..4 and iemer Sec...4-Sec..4) KECE3 Communication Systems I Lecture #3, March, 0 Prof. Young-Chai Ko 년 3 월 일일요일 Review Signal classification Phasor signal and spectra Representation

More information

Homework 3 Solutions

Homework 3 Solutions EECS Signals & Systems University of California, Berkeley: Fall 7 Ramchandran September, 7 Homework 3 Solutions (Send your grades to ee.gsi@gmail.com. Check the course website for details) Review Problem

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

EE 438 Supplementary Notes on Fourier Series and Linear Algebra.

EE 438 Supplementary Notes on Fourier Series and Linear Algebra. EE 38 Supplementary Notes on Fourier Series and Linear Algebra. Discrete-Time Fourier Series. How to write a vector s as a sum where {g,...,g m } are pairwise orthogonal? s m a k g k, k Answer: project

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

(Refer Slide Time: 01:30)

(Refer Slide Time: 01:30) Networks and Systems Prof V.G K.Murti Department of Electrical Engineering Indian Institute of Technology, Madras Lecture - 11 Fourier Series (5) Continuing our discussion of Fourier series today, we will

More information

The Fourier Transform (and more )

The Fourier Transform (and more ) The Fourier Transform (and more ) imrod Peleg ov. 5 Outline Introduce Fourier series and transforms Introduce Discrete Time Fourier Transforms, (DTFT) Introduce Discrete Fourier Transforms (DFT) Consider

More information

SEISMIC WAVE PROPAGATION. Lecture 2: Fourier Analysis

SEISMIC WAVE PROPAGATION. Lecture 2: Fourier Analysis SEISMIC WAVE PROPAGATION Lecture 2: Fourier Analysis Fourier Series & Fourier Transforms Fourier Series Review of trigonometric identities Analysing the square wave Fourier Transform Transforms of some

More information

Time and Spatial Series and Transforms

Time and Spatial Series and Transforms Time and Spatial Series and Transforms Z- and Fourier transforms Gibbs' phenomenon Transforms and linear algebra Wavelet transforms Reading: Sheriff and Geldart, Chapter 15 Z-Transform Consider a digitized

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

King Fahd University of Petroleum & Minerals Computer Engineering Dept

King Fahd University of Petroleum & Minerals Computer Engineering Dept King Fahd University of Petroleum & Minerals Computer Engineering Dept COE 4 Data and Computer Communications erm 5 Dr. shraf S. Hasan Mahmoud Rm -4 Ext. 74 Email: ashraf@kfupm.edu.sa /7/6 Dr. shraf S.

More information

Print Name : ID : ECE Test #1 9/22/2016

Print Name :  ID : ECE Test #1 9/22/2016 Print Name : Email ID : ECE 2660 Test #1 9/22/2016 All answers must be recorded on the answer page (page 2). You must do all questions on the exam. For Part 4 you must show all your work and write your

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

Summary of lecture 1. E x = E x =T. X T (e i!t ) which motivates us to define the energy spectrum Φ xx (!) = jx (i!)j 2 Z 1 Z =T. 2 d!

Summary of lecture 1. E x = E x =T. X T (e i!t ) which motivates us to define the energy spectrum Φ xx (!) = jx (i!)j 2 Z 1 Z =T. 2 d! Summary of lecture I Continuous time: FS X FS [n] for periodic signals, FT X (i!) for non-periodic signals. II Discrete time: DTFT X T (e i!t ) III Poisson s summation formula: describes the relationship

More information

Discrete-Time Fourier Transform

Discrete-Time Fourier Transform Discrete-Time Fourier Transform Chapter Intended Learning Outcomes: (i) (ii) (iii) Represent discrete-time signals using discrete-time Fourier transform Understand the properties of discrete-time Fourier

More information

L6: Short-time Fourier analysis and synthesis

L6: Short-time Fourier analysis and synthesis L6: Short-time Fourier analysis and synthesis Overview Analysis: Fourier-transform view Analysis: filtering view Synthesis: filter bank summation (FBS) method Synthesis: overlap-add (OLA) method STFT magnitude

More information

Fourier Series : Dr. Mohammed Saheb Khesbak Page 34

Fourier Series : Dr. Mohammed Saheb Khesbak Page 34 Fourier Series : Dr. Mohammed Saheb Khesbak Page 34 Dr. Mohammed Saheb Khesbak Page 35 Example 1: Dr. Mohammed Saheb Khesbak Page 36 Dr. Mohammed Saheb Khesbak Page 37 Dr. Mohammed Saheb Khesbak Page 38

More information

Digital Band-pass Modulation PROF. MICHAEL TSAI 2011/11/10

Digital Band-pass Modulation PROF. MICHAEL TSAI 2011/11/10 Digital Band-pass Modulation PROF. MICHAEL TSAI 211/11/1 Band-pass Signal Representation a t g t General form: 2πf c t + φ t g t = a t cos 2πf c t + φ t Envelope Phase Envelope is always non-negative,

More information

Solutions 1-4 by Poya Khalaf

Solutions 1-4 by Poya Khalaf Solutions -4 by Poya Khalaf. Consider the function: f { t < [ e t sin(t), te 2t] T t Calculate f 2,[, ] using the time-domain definition and then using Parsevals identity. The following code has been written

More information

Poles, Zeros, and Frequency Response

Poles, Zeros, and Frequency Response Poles, Zeros, and Frequency Response With the previous circuits, you can build filters with Real poles Complex Poles, and Zeros at s = 0 Filter design uses this to places poles and zeros to give a desired

More information

ANSWERS TO SELECTED EXCERCISES, CH 4-5

ANSWERS TO SELECTED EXCERCISES, CH 4-5 ANSWERS O SELECED EXCERCISES, CH 4-5 Exercise 4.4 a. Peak detection is, in many cases, a simple process it's usually just a matter of identifying regions of your signal that rise above a certain threshold,

More information

In this Lecture. Frequency domain analysis

In this Lecture. Frequency domain analysis In this Lecture Frequency domain analysis Introduction In most cases we want to know the frequency content of our signal Why? Most popular analysis in frequency domain is based on work of Joseph Fourier

More information

Simulation, Transfer Function

Simulation, Transfer Function Max Force (lb) Displacement (in) 1 ME313 Homework #12 Simulation, Transfer Function Last Updated November 17, 214. Repeat the car-crash problem from HW#6. Use the Matlab function lsim with ABCD format

More information

The Discrete Fourier Transform (DFT) Properties of the DFT DFT-Specic Properties Power spectrum estimate. Alex Sheremet.

The Discrete Fourier Transform (DFT) Properties of the DFT DFT-Specic Properties Power spectrum estimate. Alex Sheremet. 4. April 2, 27 -order sequences Measurements produce sequences of numbers Measurement purpose: characterize a stochastic process. Example: Process: water surface elevation as a function of time Parameters:

More information

Ver 3808 E1.10 Fourier Series and Transforms (2014) E1.10 Fourier Series and Transforms. Problem Sheet 1 (Lecture 1)

Ver 3808 E1.10 Fourier Series and Transforms (2014) E1.10 Fourier Series and Transforms. Problem Sheet 1 (Lecture 1) Ver 88 E. Fourier Series and Transforms 4 Key: [A] easy... [E]hard Questions from RBH textbook: 4., 4.8. E. Fourier Series and Transforms Problem Sheet Lecture. [B] Using the geometric progression formula,

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

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

Lecture 6: Discrete Fourier Transform

Lecture 6: Discrete Fourier Transform Lecture 6: Discrete Fourier Transform In the previous lecture we introduced the discrete Fourier transform as given either by summations or as a matrix vector product The discrete Fourier transform of

More information

DFT Octave Codes (0B) Young Won Lim 4/15/17

DFT Octave Codes (0B) Young Won Lim 4/15/17 Copyright (c) 2009-2017 Young W. Lim. Permission is granted to copy, distribute and/or modify this document under the terms of the GNU Free Documentation License, Version 1.2 or any later version published

More information

Theory and Problems of Signals and Systems

Theory and Problems of Signals and Systems SCHAUM'S OUTLINES OF Theory and Problems of Signals and Systems HWEI P. HSU is Professor of Electrical Engineering at Fairleigh Dickinson University. He received his B.S. from National Taiwan University

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

Math 308 Week 8 Solutions

Math 308 Week 8 Solutions Math 38 Week 8 Solutions There is a solution manual to Chapter 4 online: www.pearsoncustom.com/tamu math/. This online solutions manual contains solutions to some of the suggested problems. Here are solutions

More information

Gabor multipliers for pseudodifferential operators and wavefield propagators

Gabor multipliers for pseudodifferential operators and wavefield propagators Gabor multipliers for pseudodifferential operators and wavefield propagators Michael P. Lamoureux, Gary F. Margrave and Peter C. Gibson ABSTRACT Gabor multipliers We summarize some applications of Gabor

More information

The Laplace Transform

The Laplace Transform The Laplace Transform Generalizing the Fourier Transform The CTFT expresses a time-domain signal as a linear combination of complex sinusoids of the form e jωt. In the generalization of the CTFT to the

More information

EE482: Digital Signal Processing Applications

EE482: Digital Signal Processing Applications Professor Brendan Morris, SEB 3216, brendan.morris@unlv.edu EE482: Digital Signal Processing Applications Spring 2014 TTh 14:30-15:45 CBC C222 Lecture 02 DSP Fundamentals 14/01/21 http://www.ee.unlv.edu/~b1morris/ee482/

More information

Stability. X(s) Y(s) = (s + 2) 2 (s 2) System has 2 poles: points where Y(s) -> at s = +2 and s = -2. Y(s) 8X(s) G 1 G 2

Stability. X(s) Y(s) = (s + 2) 2 (s 2) System has 2 poles: points where Y(s) -> at s = +2 and s = -2. Y(s) 8X(s) G 1 G 2 Stability 8X(s) X(s) Y(s) = (s 2) 2 (s 2) System has 2 poles: points where Y(s) -> at s = 2 and s = -2 If all poles are in region where s < 0, system is stable in Fourier language s = jω G 0 - x3 x7 Y(s)

More information

Discrete Time Fourier Transform (DTFT) Digital Signal Processing, 2011 Robi Polikar, Rowan University

Discrete Time Fourier Transform (DTFT) Digital Signal Processing, 2011 Robi Polikar, Rowan University Discrete Time Fourier Transform (DTFT) Digital Signal Processing, 2 Robi Polikar, Rowan University Sinusoids & Exponentials Signals Phasors Frequency Impulse, step, rectangular Characterization Power /

More information

MA 201: Differentiation and Integration of Fourier Series Applications of Fourier Series Lecture - 10

MA 201: Differentiation and Integration of Fourier Series Applications of Fourier Series Lecture - 10 MA 201: Differentiation and Integration of Fourier Series Applications of Fourier Series ecture - 10 Fourier Series: Orthogonal Sets We begin our treatment with some observations: For m,n = 1,2,3,... cos

More information

Chapter 2. Signals. Static and Dynamic Characteristics of Signals. Signals classified as

Chapter 2. Signals. Static and Dynamic Characteristics of Signals. Signals classified as Chapter 2 Static and Dynamic Characteristics of Signals Signals Signals classified as. Analog continuous in time and takes on any magnitude in range of operations 2. Discrete Time measuring a continuous

More information

Fourier Series and Transforms. Revision Lecture

Fourier Series and Transforms. Revision Lecture E. (5-6) : / 3 Periodic signals can be written as a sum of sine and cosine waves: u(t) u(t) = a + n= (a ncosπnft+b n sinπnft) T = + T/3 T/ T +.65sin(πFt) -.6sin(πFt) +.6sin(πFt) + -.3cos(πFt) + T/ Fundamental

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

Math 56 Homework 5 Michael Downs

Math 56 Homework 5 Michael Downs 1. (a) Since f(x) = cos(6x) = ei6x 2 + e i6x 2, due to the orthogonality of each e inx, n Z, the only nonzero (complex) fourier coefficients are ˆf 6 and ˆf 6 and they re both 1 2 (which is also seen from

More information

5.1. Periodic Signals: A signal f(t) is periodic iff for some T 0 > 0,

5.1. Periodic Signals: A signal f(t) is periodic iff for some T 0 > 0, 5. Periodic Sigals: A sigal f(t) is periodic iff for some >, f () t = f ( t + ) i t he smallest value that satisfies the above coditios is called the period of f(t). Cosider a sigal examied over to 5 secods

More information

Fourier Series. Spectral Analysis of Periodic Signals

Fourier Series. Spectral Analysis of Periodic Signals Fourier Series. Spectral Analysis of Periodic Signals he response of continuous-time linear invariant systems to the complex exponential with unitary magnitude response of a continuous-time LI system at

More information

Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science Electric Machines

Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science Electric Machines Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science 6.685 Electric Machines Problem Set 1 Solutions September 1, 5 Problem 1: If we assume, as suggested in the

More information

UNIVERSITI MALAYSIA PERLIS

UNIVERSITI MALAYSIA PERLIS UNIVERSITI MALAYSIA PERLIS SCHOOL OF COMPUTER & COMMUNICATIONS ENGINEERING EKT 230 SIGNALS AND SYSTEMS LABORATORY MODULE LAB 5 : LAPLACE TRANSFORM & Z-TRANSFORM 1 LABORATORY OUTCOME Ability to describe

More information

23.6. The Complex Form. Introduction. Prerequisites. Learning Outcomes

23.6. The Complex Form. Introduction. Prerequisites. Learning Outcomes he Complex Form 3.6 Introduction In this Section we show how a Fourier series can be expressed more concisely if we introduce the complex number i where i =. By utilising the Euler relation: e iθ cos θ

More information

Digital Signal Processing: Signal Transforms

Digital Signal Processing: Signal Transforms Digital Signal Processing: Signal Transforms Aishy Amer, Mohammed Ghazal January 19, 1 Instructions: 1. This tutorial introduces frequency analysis in Matlab using the Fourier and z transforms.. More Matlab

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

Fourier Representations of Signals & LTI Systems

Fourier Representations of Signals & LTI Systems 3. Introduction. A signal can be represented as a weighted superposition of complex sinusoids. x(t) or x[n] 2. LTI system: LTI System Output = A weighted superposition of the system response to each complex

More information