Solutions to Assignment 4

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

More on Fourier Series

Chapter 4 The Fourier Series and Fourier Transform

EE3210 Lab 3: Periodic Signal Representation by Fourier Series

Solutions to Problems in Chapter 4

GATE EE Topic wise Questions SIGNALS & SYSTEMS

EEL3135: Homework #3 Solutions

Assignment 3 Solutions

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

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

Frequency Analysis: The Fourier

6.003 Homework #10 Solutions

a k cos kω 0 t + b k sin kω 0 t (1) k=1

Examples of the Fourier Theorem (Sect. 10.3). The Fourier Theorem: Continuous case.

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

Math 5 Trigonometry Chapter 4 Test Fall 08 Name Show work for credit. Write all responses on separate paper. Do not use a calculator.

I. Signals & Sinusoids

Fourier Series and Fourier Transforms

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

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

(Refer Slide Time: 01:30)

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

!Sketch f(t) over one period. Show that the Fourier Series for f(t) is as given below. What is θ 1?

Time-Frequency Analysis

Fourier series. XE31EO2 - Pavel Máša. Electrical Circuits 2 Lecture1. XE31EO2 - Pavel Máša - Fourier Series

Line Spectra and their Applications

Fourier series: Additional notes

5 Trigonometric Functions

Chapter 17 : Fourier Series Page 1 of 12

Question Paper Code : AEC11T02

信號與系統 Signals and Systems

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

Chapter 4 The Fourier Series and Fourier Transform

First Order Linear Ordinary Differential Equations

Fourier Series. Department of Mathematical and Statistical Sciences University of Alberta

3 rd class Mech. Eng. Dept. hamdiahmed.weebly.com Fourier Series

Fall Exam 4: 8&11-11/14/13 - Write all responses on separate paper. Show your work for credit.

Topic 3: Fourier Series (FS)

1D Wave PDE. Introduction to Partial Differential Equations part of EM, Scalar and Vector Fields module (PHY2064) Richard Sear.

Trigonometric Identities Exam Questions

Jean-Baptiste Joseph Fourier

Math 1B Final Exam, Solution. Prof. Mina Aganagic Lecture 2, Spring (6 points) Use substitution and integration by parts to find:

ECE 301 Fall 2011 Division 1. Homework 1 Solutions.

Mathematical Methods: Fourier Series. Fourier Series: The Basics

EE301 Signals and Systems In-Class Exam Exam 3 Thursday, Apr. 19, Cover Sheet

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

Differential Equations: Homework 8

5.3 SOLVING TRIGONOMETRIC EQUATIONS

SIGNALS AND SYSTEMS: PAPER 3C1 HANDOUT 6a. Dr David Corrigan 1. Electronic and Electrical Engineering Dept.

DISCRETE-TIME TIME-VARYING ROBUST STABILIZATION FOR SYSTEMS IN POWER FORM. Dina Shona Laila and Alessandro Astolfi

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

Assignment #09 - Solution Manual

(e) (i) Prove that C(x) = C( x) for all x. (2)

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

Name (print): Lab (circle): W8 Th8 Th11 Th2 F8. θ (radians) θ (degrees) cos θ sin θ π/ /2 1/2 π/4 45 2/2 2/2 π/3 60 1/2 3/2 π/

Date: 1 April (1) The only reference material you may use is one 8½x11 crib sheet and a calculator.

Discrete Systems & Z-Transforms. Week Date Lecture Title. 9-Mar Signals as Vectors & Systems as Maps 10-Mar [Signals] 3

SOLUTIONS to ECE 2026 Summer 2018 Problem Set #3

Algebra II B Review 5

Mathematics 2203, Test 1 - Solutions

Date: 31 March (1) The only reference material you may use is one 8½x11 crib sheet and a calculator.

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

Chapter 17: Fourier Series

Worksheet Week 7 Section

Fourier Series, Fourier Transforms, and Periodic Response to Periodic Forcing

Differential Equations

GENERAL I ARTICLE. Fourier Series. The Mathematics of Periodic Phenomena. S Thangavelu. k=o

MATH section 3.1 Maximum and Minimum Values Page 1 of 7

Part: Frequency and Time Domain

f = 1 T 6 a.c. (Alternating Current) Circuits Most signals of interest in electronics are periodic : they repeat regularly as a function of time.

IB Paper 6: Signal and Data Analysis

Discrete-time Fourier transform (DTFT) representation of DT aperiodic signals Section The (DT) Fourier transform (or spectrum) of x[n] is

EE 435. Lecture 30. Data Converters. Spectral Performance

GEORGIA INSTITUTE OF TECHNOLOGY SCHOOL OF ELECTRICAL AND COMPUTER ENGINEERING

Math Section 4.3 Unit Circle Trigonometry

AP Calculus BC - Problem Solving Drill 19: Parametric Functions and Polar Functions

A. Incorrect! For a point to lie on the unit circle, the sum of the squares of its coordinates must be equal to 1.

QUESTION BANK SIGNALS AND SYSTEMS (4 th SEM ECE)

In this Lecture. Frequency domain analysis

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

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

Math 345: Applied Mathematics

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

Representing a Signal

A basic trigonometric equation asks what values of the trig function have a specific value.

HILBERT SPACES AND FOURIER SERIES

ENGIN 211, Engineering Math. Fourier Series and Transform

Continuous-time Fourier Methods

3 Fourier Series Representation of Periodic Signals

4-3 Trigonometric Functions on the Unit Circle

chap5_fourier_series_lr_circuit.doc 1/18 Consider the rectangular pulse train of example 3.2 of the text as the input to the series LR circuit.

Parametric Curves You Should Know

Superposition (take 3)

Solution to Tutorial 5 Isolated DC-DC Converters & Inverters

Fourier Series. Fourier Transform

natural frequency of the spring/mass system is ω = k/m, and dividing the equation through by m gives

The Fourier series are applicable to periodic signals. They were discovered by the

Summer Assignment MAT 414: Calculus

Properties of Fourier Series - GATE Study Material in PDF

LECTURE 12 Sections Introduction to the Fourier series of periodic signals

Transcription:

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 is =. Using Euler s relation one has: sin(t 3) = sin( 3) = ( e ( ) e ) ( ) = e e t e3 e t sin(6t) = sin(3 t) = ( e 3 t e ) 3 t = e3 t e 3 t x(t) = e 3 t e3 e t + e e t + e3 t From Equation (9), the nonzero Fourier series coefficients a k are identified to be: a = = = e( ) a = e3 = e3 = e ( +3) = e (3 3 ) = e.7 a = e = e = e [ ( +3)] = e ( 3 ) = e.7 a 3 = = = e( ) [3] (b) With a a k e θ k, then ak and θ k are the magnitude and phase of a k, respectively. Also, as a convention, the phase angles are always converted to the range [, ] by adding (or subtracting) with multiples of. The magnitude and phase spectrum of x(t) are sketched in Figure and. Note that the magnitude spectrum is even and the phase spectrum is odd. This is expected since x(t) is a real-valued signal. Remark: This question is accidentally given to be the same as the example discussed in class as well as in Lecture Notes (page ). (9) [5]. A continuous-time periodic signal x(t) is real-valued and has a fundamental period T = 8 the fundamental frequency is =. The nonzero Fourier series coefficients for x(t) are specified as: a = a =, a 5 = a 5 = x(t) = k= a k e k t = (e 5 t + e 5 t ) + (e t e t ) = cos(5 t) sin( t) = cos ( t + ) + cos(5 t) Electrical Engineering, University of Saskatchewan Page 6

EE35 Spectrum Analysis and Discrete Time Systems (Fall 5) Magnitude Spectrum.5 5 5 Phase Spectrum 5 5 Normalized Frequency (/ ) Figure : Magnitude spectrum of x(t). Comparing the terms gives:, α, 5 ; φ, otherwise 3. (Properties of Fourier Series Coefficients) {,, otherwise ; k = k,,,... [] (a) Signals (i) and (ii) are real-valued since their magnitude spectra are even and phase spectra are odd. Signal (iii) is a complex-valued since its phase spectrum is not odd. [] (b) Since e ± = and e =, the FS coefficients of signal (ii) are real-valued. Thus signal (ii) is both real-valued and even function. None of the signal is both real-valued and odd since an real-valued and odd signal must have an odd phase spectrum and the phase values can only be, / and / only. [] (c) Because signal (i) is a real-valued signal, any form of FS can be used to write x(t). For example, x(t) = e e t + e / e t + + e / e t + e e t [ ( = + cos t + ) ] + cos ( t + ) Obviously, the dc component is a = volt. The average power is simply found by applying Parseval s relation: k= a k = + + + + = watts. Electrical Engineering, University of Saskatchewan Page 7

EE35 Spectrum Analysis and Discrete Time Systems (Fall 5) (i) 3 3 (ii) 3 3 (iii) 3 3. (Fourier series of the sawtooth waveform) [] (a) The fundamental period is T = and the fundamental frequency is = T =. [3] (b) To compute the trigonometric Fourier series coefficients B k and C k, consider x(t) in one period, from t. Then { t, t < x(t) =, < t Electrical Engineering, University of Saskatchewan Page 8

EE35 Spectrum Analysis and Discrete Time Systems (Fall 5) Similarly B T x(t) cos(k t)dt = T = [ cos(kt) + t ] (k) k sin(kt) C T x(t) sin(k t)dt = T = [ sin(kt) t ] (k) k cos(kt) t cos(kt)dt = ( )k (k) t sin(kt)dt = ( )k k The DC component of x(t) is simply a = T T x(t)dt = t d t = t = [3] (c) The magnitude and phase spectrum of x(t) are plotted in Figure 5. Recall that the magnitude spectrum is the plot of a k = Bk + C k, while the phase spectrum is the plot of a tan (C k /B k ). Again, notice that since x(t) is a real function, it has even amplitude and odd phase spectrum..3 Magnitude Spectrum... 5 5 Phase Spectrum 5 5 Normalized Frequency (/ ) Figure 5: Magnitude spectrum of x(t). Electrical Engineering, University of Saskatchewan Page 9

EE35 Spectrum Analysis and Discrete Time Systems (Fall 5) [3] (d) Consider the following approximation for x(t): N ˆx(t) = a + [B k cos(k t) C k sin(k t)] k= Note the Gibb s phe- Plots of ˆx(t) for N = 5,, 5 are shown in Figure 6. nomenon at the points of discontinuity..5 N=5 3.5 N= 3.5 N=5 3 t (sec) Figure 6: Partial Fourier series approximations of x(t) with N = 5,, 5. [3] (e) The average power of x(t) can be computed as P T = x (t)dt = t dt = t3 T T 6 = 6 Using Matlab, the smallest values of N in the above approximation such that ˆx(t) captures 95% and 99% power in x(t) are found to be N = 6 and N = 3, respectively. The Matlab program is listed below. P_x=/6;a=/;w=pi; percentage=.95;p_xhat=a^;k=; while P_xhat<percentage*P_x k=k+; ak=((-).^k-)./(*(k*pi).^)+*(-).^k./(*pi*k); P_xhat=P_xhat+*(abs(ak))^; end N=k; Electrical Engineering, University of Saskatchewan Page