Chapter 2 : Fourier Series. Chapter 3 : Fourier Series

Similar documents
Chapter 4 The Fourier Series and Fourier Transform

Chapter One Fourier Series and Fourier Transform

EECS 2602 Winter Laboratory 3 Fourier series, Fourier transform and Bode Plots in MATLAB

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes

ME 452 Fourier Series and Fourier Transform

6.003 Homework #9 Solutions

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes

6.003 Homework #9 Solutions

III-A. Fourier Series Expansion

Spectral Analysis. Joseph Fourier The two representations of a signal are connected via the Fourier transform. Z x(t)exp( j2πft)dt

Voltage/current relationship Stored Energy. RL / RC circuits Steady State / Transient response Natural / Step response

CHAPTER 2 Signals And Spectra

Chapters 6 & 7: Trigonometric Functions of Angles and Real Numbers. Divide both Sides by 180

6.003: Signals and Systems. Fourier Representations

6.003 Homework #8 Solutions

SINUSOIDAL WAVEFORMS

Delhi Noida Bhopal Hyderabad Jaipur Lucknow Indore Pune Bhubaneswar Kolkata Patna Web: Ph:

Some Basic Information about M-S-D Systems

Signal and System (Chapter 3. Continuous-Time Systems)

Wall. x(t) f(t) x(t = 0) = x 0, t=0. which describes the motion of the mass in absence of any external forcing.

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

Traveling Waves. Chapter Introduction

DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING EXAMINATIONS 2008

EECS20n, Solution to Midterm 2, 11/17/00

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is

10. State Space Methods

MATH 31B: MIDTERM 2 REVIEW. x 2 e x2 2x dx = 1. ue u du 2. x 2 e x2 e x2] + C 2. dx = x ln(x) 2 2. ln x dx = x ln x x + C. 2, or dx = 2u du.

V L. DT s D T s t. Figure 1: Buck-boost converter: inductor current i(t) in the continuous conduction mode.

Laplace Transform and its Relation to Fourier Transform

ADDITIONAL PROBLEMS (a) Find the Fourier transform of the half-cosine pulse shown in Fig. 2.40(a). Additional Problems 91

8. Basic RL and RC Circuits

Q1) [20 points] answer for the following questions (ON THIS SHEET):

EECE 301 Signals & Systems Prof. Mark Fowler

SOLUTIONS TO ECE 3084

6.003 Homework #13 Solutions

Differential Equations

6.2 Transforms of Derivatives and Integrals.

Outline Chapter 2: Signals and Systems

6.003: Signals and Systems. Relations among Fourier Representations

Hilbert Inner Product Space (2B) Young Won Lim 2/23/12

Chapter 7: Solving Trig Equations

Representing a Signal. Continuous-Time Fourier Methods. Linearity and Superposition. Real and Complex Sinusoids. Jean Baptiste Joseph Fourier

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

About the HELM Project HELM (Helping Engineers Learn Mathematics) materials were the outcome of a three-year curriculum development project

Sample Final Exam (finals03) Covering Chapters 1-9 of Fundamentals of Signals & Systems

A complex discrete (or digital) signal x(n) is defined in a

6.302 Feedback Systems Recitation 4: Complex Variables and the s-plane Prof. Joel L. Dawson

Fundamentals of Electrical Engineering 3

15. Vector Valued Functions

Notes 04 largely plagiarized by %khc

2.4 Cuk converter example

Chapter 1 Fundamental Concepts

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3

Basic Circuit Elements Professor J R Lucas November 2001

Section 7.4 Modeling Changing Amplitude and Midline

δ (τ )dτ denotes the unit step function, and

Chapter 2: Principles of steady-state converter analysis

NCSS Statistical Software. , contains a periodic (cyclic) component. A natural model of the periodic component would be

Math 2214 Solution Test 1A Spring 2016

!!"#"$%&#'()!"#&'(*%)+,&',-)./0)1-*23)

ES.1803 Topic 22 Notes Jeremy Orloff

6.003: Signals and Systems

System Processes input signal (excitation) and produces output signal (response)

From Complex Fourier Series to Fourier Transforms

Lab 10: RC, RL, and RLC Circuits

Mon Apr 9 EP 7.6 Convolutions and Laplace transforms. Announcements: Warm-up Exercise:

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes

Two Coupled Oscillators / Normal Modes

Math Final Exam Solutions

EEEB113 CIRCUIT ANALYSIS I

14 Autoregressive Moving Average Models

Chapter 7 Response of First-order RL and RC Circuits

Structural Dynamics and Earthquake Engineering

LAPLACE TRANSFORM AND TRANSFER FUNCTION

AP Calculus BC Chapter 10 Part 1 AP Exam Problems

Module 2 F c i k c s la l w a s o s f dif di fusi s o i n

RC, RL and RLC circuits

Circuit Variables. AP 1.1 Use a product of ratios to convert two-thirds the speed of light from meters per second to miles per second: 1 ft 12 in

Second-Order Differential Equations

Guest Lectures for Dr. MacFarlane s EE3350 Part Deux

dt = C exp (3 ln t 4 ). t 4 W = C exp ( ln(4 t) 3) = C(4 t) 3.

Vehicle Arrival Models : Headway

5.1 - Logarithms and Their Properties

4.1 - Logarithms and Their Properties

EELE Lecture 3,4 EE445 - Outcomes. Physically Realizable Waveforms. EELE445 Montana State University. In this lecture you:

Week 1 Lecture 2 Problems 2, 5. What if something oscillates with no obvious spring? What is ω? (problem set problem)

Short Introduction to Fractional Calculus

ECE 2100 Circuit Analysis

Linear Response Theory: The connection between QFT and experiments

Reading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4.

ENGI 9420 Engineering Analysis Assignment 2 Solutions

Math 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities:

Robotics I. April 11, The kinematics of a 3R spatial robot is specified by the Denavit-Hartenberg parameters in Tab. 1.

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson

Answers to 1 Homework

A Bayesian Approach to Spectral Analysis

Signals and Systems Profs. Byron Yu and Pulkit Grover Fall Midterm 1 Solutions

Lecture 2: Optics / C2: Quantum Information and Laser Science

Lecture Notes 2. The Hilbert Space Approach to Time Series

Echocardiography Project and Finite Fourier Series

Transcription:

Chaper 2 : Fourier Series.0 Inroducion Fourier Series : represenaion of periodic signals as weighed sums of harmonically relaed frequencies. If a signal x() is periodic signal, hen x() can be represened in erms of Fourier Series eiher in : a) Trigonomeric Form b) Exponenial (Complex) Form Fourier Series Saw ooh waveform Infinie number of sine waves (harmonics) Chaper 3 : Fourier Series. Trigonomeric Fourier Series General equaion : x() is expressed as he sum of sinusoidal componens having differen frequencies where : * a n and b n : he Fourier coefficiens * a 0 : DC Value

Chaper 3 : Fourier Series Express he following signal x() as shown in figure below as Trigonomeric Fourier Series: x() -T -0.5T 0 0.5T T - Chaper 3 : Fourier Series Express he following signal x() as shown in figure below as Trigonomeric Fourier Series: x() x() = / ; 0 < < 0 ; < < 2-2 - 0 2 3-2

Chaper 3 : Fourier Series Express he following signal x() as shown in figure below as Trigonomeric Fourier Series: x() -2-0 2 3 - Chaper 3 : Fourier Series.2 Symmery Properies The symmery properies can be classified ino 5 ypes : a) Even Symmery b) Odd Symmery c) Half Wave Symmery d) Even And Half Wave Symmery e) Odd And Half Wave Symmery 3

Chaper 3 : Fourier Series.2 Symmery Properies a) Even Symmery The signal x() is said o be even symmery if x() = x(-) x() x() = x(-) x() x() = x(-) Chaper 3 : Fourier Series.2 Symmery Properies b) Odd Symmery The signal x() is said o be even symmery if x() = -x(-) x() x() = -x(-) x() - - x() = x(-) 4

Chaper 3 : Fourier Series.2 Symmery Properies c) Half Wave Symmery The signal x() is said o be half wave symmery if x() = -x( + T/2) x() x() = -x(+t/2) - T/2 - x() x() = -x(+t/2) T/2 T T/2 T/2 T Chaper 3 : Fourier Series The firs half-cycle of a periodic signal is shown in figure below and he period is T = 2 sec. Skech y() clearly for 3 complee cycles if : i) y() is an even-symmerical signal ii) y() is an odd-symmerical signal iii) y() is a half-wave symmerical signal x() 5

Chaper 3 : Fourier Series Answer i) even-symmerical signal iii) odd-symmerical signal x(-) -x(-) -3-2 - 0 2 3-3 -2-0 2 3 - Chaper 3 : Fourier Series Answer iii) half-wave symmerical signal x-(+) -3-2 - 0 2 3-6

Chaper 3 : Fourier Series The firs half-cycle of a periodic signal is shown in figure below and he period is T = 4 sec. Skech y() clearly for 3 complee cycles if : i) y() is an even-symmerical signal ii) y() is an odd-symmerical signal iii) y() is a half-wave symmerical signal 3 y() 2 Chaper 3 : Fourier Series Answer i) even-symmerical signal iii) odd-symmerical signal x(-) 3 -x(-) 3-5 -4-3 -2-2 3 4 5-5 -4-3 -2-2 3 4 5 - -3 7

Chaper 3 : Fourier Series Answer iii) half-wave symmerical signal x-(+) 3-5 -4-3 -2-2 3 4 5-3 Chaper 3 : Fourier Series.2 Symmery Properies d) Even And Half-Wave Symmery Consider a half cycle signal x() shown in figure below where T = 4 sec x() - For one complee cycle, he shape of signal x() is he same properies. x(-) -x(+t/2) - - - - 8

Chaper 3 : Fourier Series.2 Symmery Properies d) Even And Half-Wave Symmery Thus, he half-wave even symmery signal x() for 3 complee cycles is shown below : x() = half-wave even -6-5 -4-3 -2-0 - 2 3 4 5 6 Chaper 3 : Fourier Series.2 Symmery Properies e) Odd And Half-Wave Symmery Consider a half cycle signal x() shown in figure below where T = 4 sec x() 2 - For one complee cycle, he shape of signal x() is he same properies. -x(-) -x(+t/2) -2-2 -2-2 - - 9

Chaper 3 : Fourier Series.2 Symmery Properies e) Odd And Half-Wave Symmery Thus, he half-wave even symmery signal x() for 3 complee cycles is shown below : x() = half-wave odd -6-5 -4-3 -2-0 - 2 3 4 5 6 Chaper 3 : Fourier Series.3 Effecs of Symmery Properies n = odd 0

Chaper 3 : Fourier Series.3 Effecs of Symmery Properies Chaper 3 : Fourier Series Express he following signal x() as shown in figure below as Trigonomeric Fourier Series using symmery propery. x() -T -0.5T 0 0.5T T -

Chaper 3 : Fourier Series Express he following signal x() as shown in figure below as Trigonomeric Fourier Series using symmery propery. x() -T -0.5T 0.5T T - Chaper 3 : Fourier Series.4 Hidden Symmery Express signal x() as TFS x() A -2T -T T 2T Soluion x() does no posses any symmery properies. 2

Chaper 3 : Fourier Series.4 Hidden Symmery Soluion However applying he hidden symmery by shifing 0.5A of he DC value for signal x() will resul signal below : g() A -2T -T 0.5A T 2T Now, signal g() posses odd symmery, hus FS of x() : x() = 0.5 A + FS of signal g() Chaper 3 : Fourier Series.4 Hidden Symmery Express signal x() as TFS x() π -3π -2π π 0 π 2π 3π 3

Chaper 3 : Fourier Series.4 Hidden Symmery Soluion Signal x() posses even-symmery propery. Thus FS of x() is : x() = π/2 + FS of signal g() x() π -3π -2π π 0 π 2π 3π Chaper 3 : Fourier Series.5 Trigonomeric Fourier Series The rigonomeric FS of signal x() is given as : Euler s Ideniy The expression ( ) can be expressed as follows : 4

Chaper 3 : Fourier Series.5 Complex Fourier Series Thus x() : Le : Then x() : Chaper 3 : Fourier Series.5 Complex Fourier Series The erm can also be represened as follows : = = Then, x() = + + 5

Chaper 2 : Fourier Series.5 Complex Fourier Series Where : where : (Euler s Ideniy) Chaper 3 : Fourier Series Express he following signal x() as shown in figure below as an Exponenial Fourier Series. x() -T -0.5T 0 0.5T T - 6

Chaper 2 : Fourier Series Express he following signal x() as shown in figure below as an Exponenial Fourier Series. x() -2T -T T 2T 3T Chaper 2 : Fourier Series The following figure below shows a half cycle of a periodic signal x(). If x() is an odd symmery signal, deermine is EFS : x() 2 2 7

Chaper 2 : Fourier Series Soluion x() is an odd symmery signal x() 2 T = 4 ω 0 = 2π / 4 = π / 2 Odd symmery -4-2 2 4 a 0 = 0 (C 0 ) a n = 0-2 b n =???? Chaper 2 : Fourier Series.6 Frequency Specrum Frequency specrum consis of : a) Ampliude specrum b) Phase specrum he plo of І C n І agains nω 0 he plo of C n agains nω 0 І C n І C n nω 0 nω 0 8

Chaper 2 : Fourier Series.6 Frequency Specrum For complex number Im (jω) І C n І a + jb Magniude, І C n І = Phase C n = C n Real (σ) Chaper 2 : Fourier Series.6 Frequency Specrum Condiions i) If b = 0, C n = a ii) If a = 0, C n = jb jω jω jb π/2 σ -π/2 -jb σ -a a І C n І = a І C n І = b C n = 0 if a > 0 (posiive) = π/2 if b > 0 (posiive) = π or π if a < 0 (negaive) = -π/2 if b < 0 (negaive) C n 9

Chaper 2 : Fourier Series Express he following signal x() as shown in figure below as an Exponenial Fourier Series. Plo he frequency specrum for signal x(). x() -T -0.5T 0 0.5T T - Chaper 2 : Fourier Series Express he following signal x() as shown in figure below as an Exponenial Fourier Series. Plo he frequency specrum of signal x(). x() -2T -T T 2T 3T 20

Chaper 2 : Fourier Series The Fourier Series of signal x() is given as : Skech he frequency specrum of x() for n = ±5, ±4, ±3, ±2, ± and 0 Chaper 2 : Fourier Series.7 TFS Coefficiens and EFS Coefficiens Relaionship or 2

Chaper 2 : Fourier Series Conver he TFS coefficiens of signal x() of figure below o EFS coefficiens. x() From previous TFS a 0 = 0 -T -0.5T 0-0.5T T a n = 0 b n = 0 ; n = even 4 / nπ ; n = odd Chaper 2 : Fourier Series Conver he TFS coefficiens of signal x() of figure below o EFS coefficiens. π x() From previous TFS a 0 = π / 2 b n = 0-3π -2π π 0 π 2π 3π a n = 0 ; n = even -4/n 2 π ; n = odd 22

Chaper 2 : Fourier Series Consider he signal y() as shown below : i) Deermine he TFS of y() ii) From he TFS of y(), wrie he EFS of y() x() 2-4 -3-2 - 0 2 3 4 - -2 23