Chapter 4: Applications of Fourier Representations. Chih-Wei Liu

Similar documents
Sampling and the Discrete Fourier Transform

Chapter 2 Sampling and Quantization. In order to investigate sampling and quantization, the difference between analog

Chapter 2: Problem Solutions

Design of Digital Filters

into a discrete time function. Recall that the table of Laplace/z-transforms is constructed by (i) selecting to get

Roadmap for Discrete-Time Signal Processing

EE 477 Digital Signal Processing. 4 Sampling; Discrete-Time

Spring 2014 EE 445S Real-Time Digital Signal Processing Laboratory. Homework #0 Solutions on Review of Signals and Systems Material

SAMPLING. Sampling is the acquisition of a continuous signal at discrete time intervals and is a fundamental concept in real-time signal processing.

5.5 Sampling. The Connection Between: Continuous Time & Discrete Time

MAHALAKSHMI ENGINEERING COLLEGE-TRICHY

LRA DSP. Multi-Rate DSP. Applications: Oversampling, Undersampling, Quadrature Mirror Filters. Professor L R Arnaut 1

5.5 Application of Frequency Response: Signal Filters

Digital Control System

Digital Control System

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

Solutions. Digital Control Systems ( ) 120 minutes examination time + 15 minutes reading time at the beginning of the exam

Properties of Z-transform Transform 1 Linearity a

Part A: Signal Processing. Professor E. Ambikairajah UNSW, Australia

Design By Emulation (Indirect Method)

4.1 Introduction. 2πδ ω (4.2) Applications of Fourier Representations to Mixed Signal Classes = (4.1)

Module 4: Time Response of discrete time systems Lecture Note 1

Lecture 10 Filtering: Applied Concepts

EE 508 Lecture 16. Filter Transformations. Lowpass to Bandpass Lowpass to Highpass Lowpass to Band-reject

RaneNote BESSEL FILTER CROSSOVER

Root Locus Diagram. Root loci: The portion of root locus when k assume positive values: that is 0

DYNAMIC MODELS FOR CONTROLLER DESIGN

Lecture 8: Period Finding: Simon s Problem over Z N

( ) ( ) ω = X x t e dt

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

Wolfgang Hofle. CERN CAS Darmstadt, October W. Hofle feedback systems

Bogoliubov Transformation in Classical Mechanics

LTV System Modelling

The Laplace Transform

Lecture 2: The z-transform

MODELING OF NEGATIVE INFLUENCES AT THE SIGNAL TRANSMISSION IN THE OPTICAL MEDIUM. Rastislav Róka, Filip Čertík

Math 201 Lecture 17: Discontinuous and Periodic Functions

Data Converters. Introduction. Overview. The ideal data converter. Sampling. x t x nt x t t nt

Digital Transmission of Analog Signals: PCM, DPCM and DM

EE/ME/AE324: Dynamical Systems. Chapter 8: Transfer Function Analysis

Lecture #9 Continuous time filter

Correction for Simple System Example and Notes on Laplace Transforms / Deviation Variables ECHE 550 Fall 2002

Question 1 Equivalent Circuits

Lecture 5 Frequency Response of FIR Systems (III)

EE 508 Lecture 16. Filter Transformations. Lowpass to Bandpass Lowpass to Highpass Lowpass to Band-reject

Nonlinear Single-Particle Dynamics in High Energy Accelerators

Fourier Series And Transforms

Given the following circuit with unknown initial capacitor voltage v(0): X(s) Immediately, we know that the transfer function H(s) is

FRTN10 Exercise 3. Specifications and Disturbance Models

CHAPTER 4 DESIGN OF STATE FEEDBACK CONTROLLERS AND STATE OBSERVERS USING REDUCED ORDER MODEL

7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281

Lecture 21. The Lovasz splitting-off lemma Topics in Combinatorial Optimization April 29th, 2004

A Study on Simulating Convolutional Codes and Turbo Codes

Advanced Digital Signal Processing. Stationary/nonstationary signals. Time-Frequency Analysis... Some nonstationary signals. Time-Frequency Analysis

Factor Analysis with Poisson Output

The type 3 nonuniform FFT and its applications

MAE140 Linear Circuits Fall 2012 Final, December 13th

A Simple Approach to Synthesizing Naïve Quantized Control for Reference Tracking

CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS

Fourier Transforms of Functions on the Continuous Domain

EE Control Systems LECTURE 6

Problem Set 8 Solutions

Determination of the local contrast of interference fringe patterns using continuous wavelet transform

Source slideplayer.com/fundamentals of Analytical Chemistry, F.J. Holler, S.R.Crouch. Chapter 6: Random Errors in Chemical Analysis

SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuits II. R 4 := 100 kohm

MATHEMATICAL MODELS OF PHYSICAL SYSTEMS

Linear System Fundamentals

Lecture 8. PID control. Industrial process control ( today) PID control. Insights about PID actions

Improving the Efficiency of a Digital Filtering Scheme for Diabatic Initialization

CHEAP CONTROL PERFORMANCE LIMITATIONS OF INPUT CONSTRAINED LINEAR SYSTEMS

A Simplified Methodology for the Synthesis of Adaptive Flight Control Systems

Real Sources (Secondary Sources) Phantom Source (Primary source) LS P. h rl. h rr. h ll. h lr. h pl. h pr

Control Systems Engineering ( Chapter 7. Steady-State Errors ) Prof. Kwang-Chun Ho Tel: Fax:

Chapter 5 Optimum Receivers for the Additive White Gaussian Noise Channel

EE Control Systems LECTURE 14

PRACTICE FINAL EXAM SOLUTION Jing Liang 12/06/2006

GNSS Solutions: What is the carrier phase measurement? How is it generated in GNSS receivers? Simply put, the carrier phase

Linear predictive coding

arxiv: v2 [math.nt] 30 Apr 2015

IEOR 3106: Fall 2013, Professor Whitt Topics for Discussion: Tuesday, November 19 Alternating Renewal Processes and The Renewal Equation

Lecture 9: Shor s Algorithm

Control Systems Analysis and Design by the Root-Locus Method

C up (E) C low (E) E 2 E 1 E 0

CHAPTER 6. Estimation

Function and Impulse Response

The Laplace Transform , Haynes Miller and Jeremy Orloff

Reading assignment: In this chapter we will cover Sections Definition and the Laplace transform of simple functions

Social Studies 201 Notes for March 18, 2005

What lies between Δx E, which represents the steam valve, and ΔP M, which is the mechanical power into the synchronous machine?

ISSN: [Basnet* et al., 6(3): March, 2017] Impact Factor: 4.116

Lecture 7: Testing Distributions

Fermi Distribution Function. n(e) T = 0 T > 0 E F

SMALL-SIGNAL STABILITY ASSESSMENT OF THE EUROPEAN POWER SYSTEM BASED ON ADVANCED NEURAL NETWORK METHOD

Mathematical modeling of control systems. Laith Batarseh. Mathematical modeling of control systems

Unbounded solutions of second order discrete BVPs on infinite intervals

Filter Dispersion. with respect to frequency otherwise signal dispersion (and thus signal distortion) will result. Right?

CDMA Signature Sequences with Low Peak-to-Average-Power Ratio via Alternating Projection

PIPELINING AND PARALLEL PROCESSING. UNIT 4 Real time Signal Processing

Massachusetts Institute of Technology Dynamics and Control II

FUNDAMENTALS OF POWER SYSTEMS

Transcription:

Chapter 4: Application of Fourier Repreentation Chih-Wei Liu

Outline Introduction Fourier ranform of Periodic Signal Convolution/Multiplication with Non-Periodic Signal Fourier ranform of Dicrete-ime Signal Sampling Recontruction of Continuou-ime Signal Dicrete-ime Proceing of Continuou-ime Signal Fourier Serie of Finite-Duration Nonperiodic Signal 2

Introduction Four clae of ignal in Fourier repreentation Continuou- and dicrete-time ignal Periodic and nonperiodc ignal In order to ue Fourier method to analyze a general ytem involving a mixing of noperiodic ay, impule repone and periodic input ignal, we mut build bridge between Fourier repreentation of different clae of ignal F/DF are mot commonly ued for analyi application We mut develop F/DF repreentation of periodic ignal DFS i the primary repreentation ued for computational application the only one can be evaluated on a computer Ue DFS to repreent the F, FS, and DF 3

F Repreentation of Periodic Signal Recall the FS repreentation of a periodic ignal xt: Note that F 2 Uing the freuency-hift property, we have Let tae the F of xt: F x e xt t F t e 2 e [ ] t 2 t t [ ] e [ ] F [ ] t F xt e [ ] 2 [ ] he F of a periodic ignal i a erie of impule paced by the fundamental freuency. he th impule ha trength 2[] he hape of i identical to that of [] 4

FS and F Repreentation of a Periodic Continuou-ime Signal 6 4 2 2 5

Example 4. F of a Coine Find the F repreentation of xt = co o t <Sol.>, co 2,. FS of xt: FS; t F 2. F of xt: co t co t 2 2 6

Example 4.2 F of a Unit Impule rain Find the F of the impule train <Sol.>. pt = periodic, fundamental period = 2. FS of pt: / t t e dt / P 2 / 2 p t t n n 3. F of pt: 2 P P 2 4 2 2 4 he F of an impule train i alo an impule train. 7

Relating the DF to the DFS 8 Recall the DFS repreentation of a periodic D ignal x[n]: Note that the invere DF of a freuency hifted impule, i.e. -, i a complex inuoid. With one period of n e, we have n DF e, 2 Let contruct an infinite erie of hifted impule eparated by 2, i.e. to obtain the following 2-periodic function 2 Let tae the DF of x[n]: x N n [ n] [ ] e N e [ ] xn n DF e m 2 m DF e 2 Since [] i N periodic and N = 2, we may combine the two um n N [ ] m m 2

Relating the DF to the DFS N [ ] n DF 2 [ ] xn e e he DF of a periodic ignal i a erie of impule paced by the fundamental freuency DFS Weighting factor = 2 DF 9 4 he DFS [] and the correponding DF e have imilar hape. 4 4 2 2 2 4

Example 4.3 DF of a Periodic Signal Determine the invere DF of the freuency-domain repreentation depicted in the following figure, where Ω = π /N. 3 2 <Sol.>. We expre one period of e a 2 2 3 4 e, 2 2 from which we infer that / 4, / 4,, otherwie on N 2 x n e e in n 2 2 2 n n 2 2. he invere DF: x[ n] N [ ] e n

Outline Introduction Fourier ranform of Periodic Signal Convolution/Multiplication with Non-Periodic Signal Fourier ranform of Dicrete-ime Signal Sampling Recontruction of Continuou-ime Signal Dicrete-ime Proceing of Continuou-ime Signal Fourier Serie of Finite-Duration Nonperiodic Signal

Convolution and Multiplication with Mixture of Periodic and Nonperiodic Signal Example: a periodic ignal fed into a table, nonperiodic impule repone Periodic input xt Stable filter Nonperiodic impule repone ht yt = xt ht 2 F i applied to continuou-time C cae DF i applied to dicrete-time D cae F For C ignal: y t x t h t Y H If xt i C periodic ignal, then x t F 2 y t x t h t Y H * F 2 [ ] y t x t h t Y H F * 2 [ ]

Convolution with Mixture of Periodic and Nonperiodic Signal y t x t h t Y H F * 2 [ ] 4 2 2 [] 2 [2] H 2 2 [] 4 2 4 Y 2 [] H 2 [2] H 2 2 4 Magnitude adutment 2 [] H 4 2 2 4 3

Example 4.4 A periodic uare wave i applied to a ytem with impule repone ht=/tint. Ue the convolution property to find the output of thi ytem. <Sol.>. he freuency repone of the LI ytem i by taing the F of the impule repone ht:, F H h t H, 2. F of the periodic uare wave: 2in / 2 2 3. he F of the ytem output i Y = H: Y 2 2 2 2 H act a a low-pa filter, paing harmonic at /2,, and /2, while uppreing all other. 4. Invere 4 F of Y: yt / 2 2 / cot / 2 2 2 2 2

Convolution with Mixture of Periodic and Nonperiodic Signal Periodic input x[n] Stable filter Nonperiodic impule repone h[n] y[n] = x[n] h[n] For D ignal: If x[n] i D periodic ignal, then N [ ] n DF 2 [ ] xn e e DF yn xn* bn Y e 2 H e [ ]. he form ofye indicate that y[n] i alo periodic with the ame period a x[n]. 5

Multiplication of Periodic and Nonperiodic Signal Continuou-time cae: Original multiplication property: F y t g t x t Y G 2 If xt i periodic. he F of xt i [ ] xt e t F 2 [ ] y t g t x t Y G [ ] F y t g t x t Y G F [ ] 6 Multiplication of gt with the periodic function xt give an F coniting of a weighted um of hifted verion of G

y t g t x t Y G F [ ] G G G Y 2 2 2 2 yt become nonperiodic ignal! he product of periodic and nonperiodic ignal i nonperiodic 7

Example 4.4 Conider a ytem with output yt = gtxt. Let xt be the uare wave and gt = cot/2, Find Y in term of G. <Sol.> FS repreentation of the uare wave: x t FS; /2 in / 2 And, we have G / 2 / 2 in / 2 Y 2 / 2 / 2 / 2 / 8

Example 4.6 AM Radio A implified AM tranmitter and receiver are depicted in Fig. 4.3a. he effect of propagation and channel noie are ignored in thi ytem. he ignal at the receiver antenna, rt, i aumed eual to the tranmitted ignal. he paband of the low-pa filter in the receiver i eual to the meage bandwidth, W < < W. Analyze thi ytem in the freuency domain. <Sol.>. he tranmitted ignal i expreed a F 9 r t m t co t R / 2 M / 2 M c c c

G 2 C 2 C R Y C C F g t r t co t G / 2 R / 2 R c c c c c G /4 M 2 /2 M /4 M 2 he original meage i recovered by low-pa filtering to remove the meage replicate centered at twice the carrier freuency. 2

Multiplication of Periodic and Nonperiodic Signal 2 Dicrete-time cae: Original multiplication property: If x[n] i periodic. he DFS of x[n] and it DF i 2 ] [ ] [ ] [ DF e Z e e Y n z n x n y [ ] 2 [ ] N n DF xn e e d e Z e Z e e Y ] [ 2 In any 2 interval of, there are exactly N multiple of the form, ince =2/N. ] [ ] [ N N e Z d e Z e Y [ ] N DF yn xnzn Y e Z e

Example 4.7 Windowing Effect Windowing or truncating: one common data-proceing application, which acce only to a portion of a data record. 7 9 Conider the ignal x n co n co n 6 6 Uing only the 2M+ value of x[n], n M, evaluate the effect of computing the DF. <Sol.>. Since hen [ ] n DF 2 [ ] N xn e e 9 7 7 9 e 6 6 which conit of impule at ± 7/6 and ± 9/6., n M 2. Define a ignal y[n] = x[n]w[n], where w n, n M 6 DF y[ n] x[ n] z[ n] Y e e Z e 2 22 Y e W e W e W e W e 2 6 9 /6 7 /6 7 /6 9 /6

3. he windowing introduce replica of We centered at the freuencie 7/6 and 9/6, intead of the impule that are preent in e. 4. We may view thi tate of affair a a mearing of broadening of the original impule 5. he energy in Ye i now meared over a band centered on the freuencie of the coine Effect of windowing a data record. Ye for different value of M, auming that = 7/6 and 2 = 9/6. a M = 8, b M = 2, c M = 8. If the number of available data point i mall relative to the freuency eparation, the DF i unable to ditinguih the preence of two ditinct 23 inuoid e.g. M=8

Fourier ranform of Dicrete-ime Signal A mixture of dicrete-time and continuou-time ignal By incorporating dicrete-time impule into the decription of the ignal in the appropriate manner. Baic concept: Conider the following ignal: xt e and gn [ ] e 24 t n Let force g[n] to be eual to the ample of xt with ample period ; i.e., g[n] = xn. e n n e i.e. = n Now, conider the DF of a D ignal x[n]: e n e xne n n x n e Define the continuou time ignal x t with the Fourier tranform : F n tn e aing the invere F of, uing the F pair. x t x n t n n

Relating the F to the DF F n, x t x n t n x n e n n x t a C ignal correpond to x[n]; Fourier tranform correpond to the C Fourier tranform e he DF e i periodic in while the F i 2/ periodic in. 2 2 2 d 25 2 2

Example 4.8 Determine the F pair aociated with the DF pair n DF xn aun e ae hi pair i derived in Example 3.7 auming that a < o the DF converge. <Sol.> n. We firt define the continuou-time ignal x t a t n 2. Uing = give F x t ae n 26

Relating the F to the DFS 27 Suppoe that x[n] i an N-periodic ignal, then Now, define x t a C ignal correpond to x[n], then the Fourier tranform of the continuou time ignal x t i [ ] 2 [ ] N n DF xn e e where [] = DFS coefficient e ] [ 2 ] [ 2 Ue the caling property of the impule, a = /a, to rewrite a 2

F 2 t x[ n] t n [ ] n. Recall that [] i N-periodic, which implie that i periodic with periodic N / = 2/ 2. Recall that x[n] i N-periodic, which implie that x t i periodic with periodic N x d 2 2 2 28 [] and x[n] are N-periodic function x t and are periodic impule train with period N and 2/. N

Outline Introduction Fourier ranform of Periodic Signal Convolution/Multiplication with Non-Periodic Signal Fourier ranform of Dicrete-ime Signal Sampling Recontruction of Continuou-ime Signal Dicrete-ime Proceing of Continuou-ime Signal Fourier Serie of Finite-Duration Nonperiodic Signal 29

Sampling We ue F repreentation of dicrete-time ignal to analyze the effect of uniformly ampling a ignal. Sampling the continuou-time ignal i often performed in order to manipulate the ignal on a computer. C ignal Sampling D ignal xn [ ] xn Let xt be a C ignal and x[n], a D ignal, i the ample of xt at integer multiple of a ampling interval. pt tn. n 3 = x t x n t n n

Sampling Proce 3 We note that hen ] [ t p t x n t t x n t t x n t n x n t n x t x n n n n 2 P t p t x t x F 2 2 = 2/ Example 4.2 An infinite um of hifted verion of the original ignal,

Sampling heorem x F t x[ n] t n n he hifted verion of may overlap with each other if i not large enough, compared with the bandwidth of, i.e. W. d d W > W 2 d 2 W < W aliaing 2 2 3 2 W 2 3 A increae or decreae, the hifted replica of move cloer together, finally 32 overlapping one another when < 2W.

Example 4.9 Conider the effect of ampling the inuoidal ignal xt co t Determine the F of the ampled ignal for = / 4. <Sol.> Recall that x F t x[ n] t n n. Firt find that 2. hen, we have which conit of pair of impule eparated by 2, centered on integer multiple of = 2/ = ¼. 33

d 2 = 4 2 2 4 d 2 /3 for = 3/2 3 2 3 2 3 3 34

Down-Sampling: Sampling Dicrete-ime Signal 35 Recall Let y[n] = x[n] be a ubampled verion of x[n], i poitive integer. Let, then F n n t n x t x ] [ ] [ ' ] [ n n n t n x n t n y t y F Y ', m m l m m l m m l Y

Down-Sampling: Sampling Dicrete-ime Signal 36 DF Y Y e Y n y ] [ ' 2 2 m m m m m m m m e Y e 2 m m e e Y F n Y n t n x t y ] [ 2 ] [ ] [ m m DF e e Y n x n y Since, therefore Ue, we have Summary

Down-Sampling by 2 e 2 2 2 2 2 2 2 4 2 2 4 2 d e 2 2 W 2 W 2 2 4 3 2 2 3 4 Figure 4.29 Effect of ubampling on the DF. a Original ignal pectrum. b m = term in E. 4.27 c m = term in E. 4.27. d m = term in E. 4.27. e Ye, auming that W < /. f Ye, auming that W > /. If the highet freuency component of e, W, i le than /, the 37 aliaing can be prevented.

Recontruction of Sampled Signal Recontruction? Not o eay!! he ample of a ignal do not alway uniuely determine the correponding continuou-time ignal 38 Nyuit Sampling heorem F Let xt be a band-limited ignal, i.e. = for > m. If > 2 m, where = 2/ i the ampling freuency, then xt i uniuely determined by it ample xn, n =,, 2,.

Ideal/Perfect Recontruction If the ignal i not band-limited, an antialiaing filter i neceary Hereafter, we conider a band-limited ignal F Suppoe that xt, then the F of the ampled ignal i 39 m a m Ideal recontruction: H r, otherwie m Ideal low-pa filter 2 : Nyuit freuency / 2 H r m / 2 Non-caual!! the perfect-recontruction cannot be implemented in any practical ytem H r

H xt x t h t / 2 H r F r / 2 h t H r r n r h t x t x t hr t x[ n] t n n r r t in 2 t in c t h x[ n] h t n r n t t n x[ n]in c t Infinite length of h r t Non-caual filter = Perfect recontruction 4

A Practical Recontruction Zero-Order Hold Filter he zero-order hold filter, which hold the input value for econd. a tair-tep approximation to the original ignal Impule repone rectangular pule:, t ho t, t, t in / 2 F /2 2 h t H e 4. A linear phae hift correponding to a time delay of /2 econd 2. A ditortion of the portion of between m and m. [he ditortion i produced by the curvature of the mainlobe of H o.] 3. Ditorted and attenuated verion of the image of, centered at nonzero multiple of.

H O m m 2 arg H O m m 2 O m m 2 econd holding for x[n] ime hift of /2 in x o t for ditortion- Stair-tep approximation main reaon for ditortion-2 & 3. Uing Eualizer for non-flattened mag. in paband 2. Uing anti-image filter Compenation filter 42 Both ditortion and 2 are reduced by increaing or, euivalently, decreaing, e.g. overampling!!

Compenation Filter he freuency repone: Hc Eualizer m m m m Anti-imaging H c, m 2in /2, m 43

Example 4.3 In thi example, we explore the benefit of overampling in recontructing a continuou-time audio ignal uing an audio compact dic player. Aume that the maximum ignal freuency i f m = 2 Hz. Conider two cae: a recontruction uing the tandard digital audio rate of / = 44. Hz, and b recontruction uing eight-time overampling, for an effective ampling rate of / 2 = 352.8 Hz. In each cae, determine the contraint on the magnitude repone of an anti-imaging filter o that the overall magnitude repone of the zero-order hold recontruction ytem i between.99 and. in the ignal paband and the image of the original ignal pectrum centered at multiple of the ampling freuency are attenuated by a factor of 3 or more. <Sol.>.99. H' c f, 2Hz f 2Hz H' f H' f o o 44

45

Outline Introduction Fourier ranform of Periodic Signal Convolution/Multiplication with Non-Periodic Signal Fourier ranform of Dicrete-ime Signal Sampling Recontruction of Continuou-ime Signal Dicrete-ime Proceing of Continuou-ime Signal Fourier Serie of Finite-Duration Nonperiodic Signal 46

Dicrete-ime Signal Proceing Several advantage for DSP algorithm Signal manipulation are more eaily performed by uing arithmetic operation of a computer than through the ue of analog component DSP ytem are eaily modified in real-time Direct dependence of the dynamic range and ignal-to-noie ratio on the number of bit ued to repreent the dicrete-time ignal Eaily implement the decimation and the interpolation H a H O Hc G 47

Sytem Repone Analyi Aume that the dicrete-time proceing operation i repreented by a D ytem with freuency repone He =, ampling interval H a HO Hc H a a a H a Y He Ha 48 Y Ho Hc He Ha

he anti-imaging filter H c eliminate freuency component above /2, hence eliminating all the term in the infinite um except for the = term. herefore, we have Y H o Hc H e Ha he overall ytem i euivalent to a continuou-time LI ytem having the repone: G H o Hc H e Ha If we chooe the anti-aliaing and anti-imaging filter uch that / H H H G H e o c a hat i, we may implement a C ytem in D by chooing ampling parameter appropriately and deigning a correponding D ytem. 49

Overampling A high ampling rate lead to high computation cot Overampling can relax the reuirement of the anti-aliaing filter a well a the anti-image filter a wide tranition band Anti-aliaing filter i ued to prevent aliaing by limiting the bandwidth of the ignal prior to ampling. W topband of filter, W t = W W width of tranition band. 5 -W -W -W > W W t = W W < -2W

Decimation wo ampled ignal x [n] and x 2 [n] with different ampling interval and 2 Sampling!! 4 2 2 4 4 2 2 4 x 2 [n] g[n] -fold pread out 5 4 2 2 4 he maximum freuency component of 2 e atifie W 2 < /

Decimation Filter Decimation filter h d [n] : a low-pa filter prevent from aliaing problem when downampling by. H d, e, otherwie 52

Interpolation Interpolation increae the ampling rate and reuire that we omehow produce value between two ample of the ignal 2 2 -fold ueeze 53 2 4 2 2 4 W W 2 Image occur!!

Interpolation Filter Decimation filter h i [n] : a low-pa filter prevent from image problem when upampling by. x[n] Upampling by Dicrete-time low pa H i e x i [n] H i, e, otherwie 2 2 54 2 2

Outline Introduction Fourier ranform of Periodic Signal Convolution/Multiplication with Non-Periodic Signal Fourier ranform of Dicrete-ime Signal Sampling Recontruction of Continuou-ime Signal Dicrete-ime Proceing of Continuou-ime Signal Fourier Serie of Finite-Duration Nonperiodic Signal 55

Why DFS for Finite Nonperiodic Signal? he primary motivation i for the numerical computation of Fourier tranform DFS i only Fourier repreentation that can be evaluated numerically!! Let x[n] be a finite-duration ignal of length M Introduce a periodic D ignal xn [ ] with period NM zero padding e M n xne n 56 2 2

Relating the DFS to the DF Conider a periodic D ignal xn [ ] with period NM, then N ~ ~ [ n ~ [ ] x n] e Apply x[n], we have [ ] N n M o = 2/N n Recall that e xne, we conclude that ~ [ ] N e n xn [ ] N M n x[ n] e he DFS coefficient of are ample of the DF of x[n], divided by N and evaluated at interval of 2/N. n 57 he effect of ampling the DF of a finite-duration nonperiodic ignal i to periodically extend the ignal in the time domain Dual to ampling in time domain In order to prevent overlap in time domain, we reuire NM, or the ampling freuency 2/M

Example 4.4 3 co n, n 3 Conider the ignal xn 8, otherwie Derive both the DF, e, and the DFS, [], of x[n], auming a period N > 3. Evaluate and plot e and N [] for N = 32, 6, and 2. <Sol.>. We rewrite the ignal x[n] a g[n]w[n], where g[n] = co3n/8 and a rectangular window wn 2. hen, n 3, otherwie DF W e e G e 2 W e e 3 / 2 in 6 in 2 3 3 /8 / 2 3 3 /8 / 2 in 6 3 8 in 6 3 8 e e e 2 in 3 8 2 2 in 3 8 2 3. Sample at = and divide by N, we have 58

e e e e e 2Ne 3 /86 3 /86 3 /86 o o o 3 /82 3 /82 3 /8 o o o 2 e e e o 2Ne e e e 3 /86 3 /86 3 /86 o o o 3 /8/2 3 /82 3 /82 3 3 /8 / 2 o in 6 o 3 8 2N in o 3 8 2 3 o 3 /8 / 2 e in 6 o 3 8 2N in o 3 8 2 o 59

Relating the FS to the F he relationhip between the FS and the F of a finite-duration nonperiodic continuou-time ignal i analogou to that of dicrete-time cae Let xt have duration, o that xt, t or t Contruct a periodic ignal xt xt m with o m Conider the FS of x t Recall that o ot o [ ] x t e dt t x t e dt D x t t x t e dt x t e t dt [ ] o he FS coefficient are ample of the F, normalized by 6