Chapter 7: The z-transform. Chih-Wei Liu

Size: px
Start display at page:

Download "Chapter 7: The z-transform. Chih-Wei Liu"

Transcription

1 Chapter 7: The -Trasform Chih-Wei Liu

2 Outlie Itroductio The -Trasform Properties of the Regio of Covergece Properties of the -Trasform Iversio of the -Trasform The Trasfer Fuctio Causality ad Stability Determiig Frequecy Respose from Poles & Zeros Computatioal Structures for DT-LTI Systems The Uilateral -Trasform

3 Itroductio The -trasform provides a broader characteriatio of discrete-time LTI systems ad their iteractio with sigals tha is possible with DTFT Sigal that is ot absolutely summable -trasform Two varieties of -trasform: Uilateral or oe-sided Bilateral or two-sided DTFT The uilateral -trasform is for solvig differece equatios with iitial coditios. The bilateral -trasform offers isight ito the ature of system characteristics such as stability, causality, ad frequecy respose. 3

4 A Geeral Complex Expoetial Complex expoetial = re j with magitude r ad agle r cos( ) jr r: dampig factor : siusoidal frequecy si( ) Re{ }: expoetial damped cosie Im{ }: expoetial damped sie < 0 expoetially damped cosie expoetially damped sie is a eigefuctio of the LTI system 4

5 Eigefuctio Property of 5 Trasfer fuctio H() is the eigevalue of the eigefuctio Polar form of H(): H() = H()e j () LTI system, h[] x[] = y[] = x[] h[] ) ( ] [ ] [ ] [ ] [ ] [ ] [ ] [ H h h x h x h y H() amplitude of H(); () phase of H() The Let = re j The LTI system chages the amplitude of the iput by H(re j ) ad shifts the phase of the siusoidal compoets by (re j ). h H. j e H y si. cos j j j j re r re H j re r re H y

6 The -Trasform x Defiitio: The -trasform of x[]: Defiitio: The iverse -trasform of X(): x x, j d. 6 A represetatio of arbitrary sigals as a weighted superpositio of eigefuctios with = re j. We obtai H ( re Hece h j ) j h[ ] r e h[ ]( re j ) j j r H re e d h[ ] r = re j d = jre j d d = (/j) d DTFT H ( re j -trasform is the DTFT of h[]r h[ ] j H ( re H ( ) j ) )( re d j ) d

7 Covergece of Laplace Trasform -trasform is the DTFT of x[]r A ecessary coditio for covergece of the -trasform is the absolute summability of x[]r : The rage of r for which the -trasform coverges is termed the regio of covergece (ROC). Covergece example: x r.. DTFT of x[]=a u[], a>, does ot exist, sice x[] is ot absolutely summable.. But x[]r is absolutely summable, if r>a, i.e. ROC, so the -trasform of x[], which is the DTFT of x[]r, does exist. 7

8 The -Plae, Poles, ad Zeros 8 To represet = re j graphically i terms of complex plae Horiotal axis of -plae = real part of ; vertical axis of -plae = imagiary part of. Relatio betwee DTFT ad -trasform: -trasform X(): the DTFT is give by the -trasform evaluated o the uit circle pole; ero c = eros of X(); d = poles of X(). j e j e The frequecy i the DTFT correspods to the poit o the uit circle at a agle with respect to the positive real axis. 0 0 N N M M a a a b b b. ~ N M d c b 0 0 / gai factor b b a

9 Example 7. Right-Sided Sigal Determie the -trasform of the sigal x u. Depict the ROC ad the locatio of poles ad eros of X() i the -plae. <Sol.> By defiitio, we have u. 0 This is a geometric series of ifiite legth i the ratio α/; X() coverges if α/ <, or the ROC is > α. Ad,,,. There is a pole at = α ad a ero at = 0 Right-sided sigal the ROC is > α. 9

10 Example 7.3 Left-Sided Sigal Determie the -trasform of the sigal y u. Depict the ROC ad the locatio of poles ad eros of Y() i the -plae. <Sol.> By defiitio, we have 0 Y Y u,,, 0 Y() coverges if /α <, or the ROC is < α. Ad,. There is a pole at = α ad a ero at = 0 Left-sided sigal the ROC is < α. Examples 7. & 7.3 reveal that the same -trasform but differet ROC. This ambiguity occurs i geeral with sigals that are oe sided

11 Properties of the ROC. The ROC caot cotai ay poles If d is a pole, the X(d) =, ad the -trasform does ot coverge at the pole. The ROC for a fiite-duratio x[] icludes the etire -plae, except possibly =0 or = For fiite-duratio x[], we might suppose that x. X() will coverge, if each term of x[] is fiite. ) If a sigal has ay oero causal compoets, the the expressio for X() will have a term ivolvig for > 0, ad thus the ROC caot iclude = 0. ) If a sigal has ay oero ocausal compoets, the the expressio for X() will have a term ivolvig for < 0, ad thus the ROC caot iclude =. 3. x[]=c[] is the oly sigal whose ROC is the etire -plae Cosider x. If 0, the the ROC will iclude = 0. If a sigal has o oero ocausal compoets ( 0), the the ROC will iclude =.

12 Properties of the ROC 4. For the ifiite-duratio sigals, the x x x. The coditio for covergece is X() <. We may write That is, we split the ifiite sum ito egative- ad positive-term portios: x ad x. 0 X ( ) Note that If I () ad I + () are fiite, the X() is guarateed to be fiite, too. A sigal that satisfies these two bouds grows o faster tha (r + ) for positive ad (r ) for egative. That is, x[ ] A ( r ), 0 (7.9) x[ ] A ( r ), 0 (7.0)

13 If the boud give i Eq. (7.9) is satisfied, the r A r A A r I () coverges if ad oly if < r. If the boud give i Eq. (7.0) is satisfied, the r A r A 0 0 I + () coverges if ad oly if > r +. = Hece, if r + < < r, the both I + () ad I () coverge ad X() also coverges. Note that if r + > r, the the ROC = For sigals x[] satisfy the expoetial bouds of Eqs. (7.9) ad (7.0), we have (). The ROC of a right-sided sigal is of the form > r +. (). The ROC of a left-sided sigal is of the form < r. (3). The ROC of a two-sided sigal is of the form r + < < r. 3

14 A right-sided sigal has a ROC of the form > r +. A left-sided sigal has a ROC of the form < r. A two-sided sigal has a ROC of the form r + < < r. 4

15 Example 7.5 Idetify the ROC associated with -trasform for each of the followig sigal: / /4 ; / y u (/4) u x u u w / u (/4) u. <Sol.> The first series coverge for </, while the secod coverge for >/4. So, the ROC is /4 < < /. Hece,. 5 Y, ; Poles at = / ad = /4 The first series coverge for >/, while the secod coverge for > /4. Hece, the ROC is > /, ad Y, Poles at = / ad = /4 4

16 0 0 4, 4 3. W 0 0 The first series coverge for < /, while the secod coverge for < ¼. So, the ROC is < /4, ad W 4, Poles at = / ad = /4 This example illustrates that the ROC of a two-side sigal (a) is a rig, i.e. i betwee the poles, the ROC of a right sided sigal (b) is the exterior of a circle, ad the ROC of a left-sided sigal (c) is the iterior of a circle. I each case the poles defie the boudaries of the ROC. 6

17 Outlie Itroductio The -Trasform Properties of the Regio of Covergece Properties of the -Trasform Iversio of the -Trasform The Trasfer Fuctio Causality ad Stability Determiig Frequecy Respose from Poles & Zeros Computatioal Structures for DT-LTI Systems The Uilateral -Trasform 7

18 Properties of the -Trasform 8 Most properties of the -trasform are aalogous to those of the DTFT. Assume that Liearity: Time Reversal: Time Shift: Z, with ROC x Z, with ROC y x R y Y R Z, with ROC at least x y ax by a by R R The ROC ca be larger tha the itersectio if oe or more terms i x[] or y[] cacel each other i the sum. x [ ] X (/ ), with ROC / Time reversal, or reflectio, correspods to replacig by. Hece, if R x is of the form a < < b, the ROC of the reflected sigal is a < / < b, or /b < < /a. Z 0 x0, with ROC Rx, except possibly 0 or. Multiplicatio by o itroduces a pole of order o at = 0 if o > 0.. If o < 0, the multiplicatio by o itroduces o poles at. If they are ot caceled by eros at ifiity i X(), the the ROC of ox() caot iclude <. R x

19 Properties of the -Trasform Multiplicatio by a Expoetial Sequece: x, with ROC Rx Is a complex umber.if X() cotais a factor (d ) i the deomiator, so that d is pole, the X(/) has a factor (d ) i the deomiator ad thus has a pole at d.. If c is a ero of X(), the X(/) has a ero at c. The poles ad eros of X() have their radii chaged by i X(/), as well as their agles are chaged by arg{} i X(/) X() X(/) 9

20 Properties of the -Trasform Covolutio: Z, with ROC at least x y x y Y R R Covolutio of time-domai sigals correspods to multiplicatio of -trasforms. The ROC may be larger tha the itersectio of R x ad R y if a pole-ero cacellatio occurs i the product X()Y(). Differetiatio i the -Domai: d x R d Z, with ROC x Multiplicatio by i the time domai correspods to differetiatio with respect to ad multiplicatio of the result by i the -domai. This operatio does ot chage the ROC. 0

21 Example 7.6 Suppose 3 Z x u u, Z y u u Y 4 Evaluate the -trasform of ax[] + by[]. <Sol.> Z ax by a b ,. ad I geeral, the ROC is the itersectio of idividual ROCs However, whe a = b: We see that the term (/) u[] has be caceled i ax[] + by[]. a ay a The pole at =/ is caceled!! the ROC elarges

22 Example 7.7 Fid the -trasform of the sigal x u u <Sol.> 4 u, with ROC First, we ow that Apply the -domai differetiatio property, we have d w u W, with ROC d Next, we ow that Apply the time-reversal property, we have y Z u [ ], with ROC 4 /4 4, with ROC 4 Z Y Last, we apply the covolutio property to obtai X(), i.e. Z, with ROC w y x w y W Y R R 4 4, X( ), with ROC 4,

23 Example 7.8 Fid the -trasform of x a cos 0u, where a is real ad positive. <Sol.> Let y[] = α u[]. The we have the -trasform Y, a Now we rewrite x[] as the sum with ROC a. j 0 j0 x e y e y The, apply the property of multiplicatio by a complex expoetial, we have j 0 j0 Y e Y e, with ROC a j0 j0 ae ae j0 j0 ae ae j 0 j 0 ae ae acos 0, acos a with ROC a. 3 0

24 Iversio of the -Trasform Direct evaluatio of the iversio itegral for iversio of the -trasform requires the complex variable theory We apply the method of partial-fractio expressio, based o -trasform pairs ad -trasform properties, to iverse trasform. The iverse trasform ca be obtaied by expressig X() as a sum of terms for which we already ow the time fuctio, which relies o the property of the ROC A right-/left- sided time sigal has a ROC that lies outside/iside the pole radius M B b0 b bm a ratioal fuctio of N A a a a M < N Suppose that 4 0 If M N, we may use log divisio to express X() as. Usig the time-shift property ad the pair We obtai M N 0 f [ ] M N 0 f N Z [ ] X ( ) ~ B( ) A( ) M N f 0

25 Iversio by Partial-Fractio Expasio. Factor the deomiator polyomial as a product of pole factors to obtai 5 b 0 b a N 0 b Case I, If all poles d are distict: N Case II: If a pole d i is repeated r times: Ai Ai A ir,,, d d d d M M, M < N. A d A A d u, with ROC d d A A d u, with ROC d d or r i i. If the ROC is of the form > d i, the the right-sided iverse -trasform is chose: i m m Z A A d u, with ROC d! m d i Appedix B!! i

26 Iversio by Partial-Fractio Expasio Case II: If a pole d i is repeated r times:. If the ROC is of the form < d i, the the left-sided iverse -trasform is chose: i m m A A d u, with ROC d! m d i i Example 7.9 Fid the iverse -trasform of, with ROC <Sol.> By partial fractio expasio, we obtai 6. right-sided left-sided x u u u.

27 Example Fid the iverse -trasform of , with ROC 4 <Sol.> Sice 3>,, First, covert X() ito a ratio of polyomials i , with ROC W ) ( W left-sided. 3 3 u u w w[] Fially, apply the time-shift property to obtai w x. 3 3 u u x

28 Remars Causality, stability, or the existece of the DTFT is sufficiet to determie the iverse trasform Causality: If a sigal is ow to be causal, the the right-sided iverse trasforms are chose Stability: If a sigal is stable, the it is absolutely summable ad has a DTFT. Hece, stability ad the existece of the DTFT are equivalet coditios. I both cases, the ROC icludes the uit circle i the -plae, =. The iverse - trasform is determied by comparig the locatios of the poles with the uit circle. If a pole is iside the uit circle, the the right-sided iverse -trasform is chose; if a pole is outside the uit circle, the the left-sided iverse - trasform is chose 8

29 Iversio by Power Series Expasio 9 Oly oe-sided sigal is applicable! Express X() as a power series i or i. Ex 7. Fid the iverse -trasform of. If the ROC is < a, the we express X() as power series i, so that we obtai a right-sided sigal.. If the ROC is > a, the we express X() as power series i, so that we obtai a left-sided sigal., with ROC X... 3 x This may ot lead to a closed-form expressio!!

30 Example 7. A advatage of the power series approach is the ability to fid iverse -trasforms for sigals that are ot a ratio of polyomials i. Fid the iverse -trasform of X( ) e, with ROC all except <Sol.> Usig the power series represetatio for e a : Thus ( ) ( ) X ( ) 0!!! [ ] [ x[ ] [ ]!! x[ ] ( 0, 0 or odd, )! otherwise e a a 0! 4] 30

31 Outlie Itroductio The -Trasform Properties of the Regio of Covergece Properties of the -Trasform Iversio of the -Trasform The Trasfer Fuctio Causality ad Stability Determiig Frequecy Respose from Poles & Zeros Computatioal Structures for DT-LTI Systems The Uilateral -Trasform 3

32 The Trasfer Fuctio 3 Recall that the trasfer fuctio H() of a LTI system is If we tae the -trasform of both sides of y[], the From differece equatio: This defiitio applies oly at values of for which X[] 0 After Substitutig for x[] ad H() for y[], we obtai ratioal trasfer fuctio Kowledge of the poles d, eros c, ad factor completely determie the system LTI system, h[] x[] = y[] = x[] h[] = re j h H X H Y X Y H M K K x b y a 0 0 M K N K b H a 0 0 ) ( ) ( ) ( ~ ) ( d c b H N M N M a b H 0 0 ) ( 0 0 ~ a b b

33 Example 7.3 Fid the trasfer fuctio ad impulse respose of a causal LTI system if the iput to the system is x (/ 3) u ad the output is y 3( ) u (/ 3) u <Sol.> The -trasforms of the iput ad output are respectively give by 3 X ( ), ROC 3 ad Y ( ), ROC ( 3) ( 3) Hece, the trasfer fuctio is The impulse respose of the system is obtai by fidig the iverse -trasform of H(). Applyig a partial fractio expasio to H() yields H( ), with ROC (/3) 33 4( ( 3) ) H ( ), ( )( ( 3) ) h ROC ( ) u (/ 3) u

34 Examples 7.4 & 7.5 Determie the trasfer fuctio ad the impulse respose for the causal LTI system described by y ( / 4) y (3/ 8) y x x <Sol.> We first obtai the trasfer fuctio by taig the -trasform: H( ) H ( ) (/4) (3/8) (/ ) (3/ 4) The system is causal, so we choose the right-side iverse -trasform for each term to obtai the followig impulse respose: <Sol.> h ( / ) u (3/ 4) u Fid the differece-equatio descriptio of a LTI system with trasfer fuctio 5 H ( ) 3 We rewrite H() as a ratio of polyomials i : y 5 H ( ) ( 3 ) 3y[ ] y[ ] 5x x 34

35 Causality ad Stability The impulse respose h(t) is the iverse LT of the trasfer fuctio H() Causality right-sided iverse -trasform Expoetially decayig term Pole d iside the uit circle, i.e., d < Stability the ROC icludes uit circle i -plae Expoetially icreasig term Causal system Pole d iside the uit circle, i.e., d < 35 No-caucal system Pole d outside the uit circle, i.e., d >

36 Causal ad Stable LTI System To obtai a uique iverse trasform of H(), we must ow the ROC or have other owledge(s) of the impulse respose The relatioships betwee the poles, eros, ad system characteristics ca provide some additioal owledges Systems that are stable ad causal must have all their poles iside the uit circle of the -plae: 36

37 Example 7.6 A LTI system has the trasfer fuctio H ( ) j j e 0.9e Fid the impulse respose, assumig that the system is (a) stable, or (b) causal. (c) Ca this system both stable ad causal? <Sol.> a. If the system is stable, the the ROC icludes the uit circle. The two cojugate poles iside the uit circle cotribute the right-sided term to the impulse respose, while the pole outside the uit circle cotributes a left-sided term. j j 4 4 h( ) (0.9e ) u[ ] (0.9e ) u[ ] 3( ) u[ ] 4(0.9) cos( ) u[ ] 3( ) u[ ] 4 b. If the system is causal, the all poles cotribute right-sided terms to the impulse respose. j j 4 4 h( ) (0.9e ) u[ ] (0.9e ) u[ ] 3( ) 4(0.9) cos[ ] u[ ] 3( ) u[ ] c. the 37 LTI system caot 4 be both stable ad causal, sice there is a pole outside the uit circle. u[ ] 3

38 Example 7.7 The first-order recursive equatio y[ ] y[ ] x[ ] may be used to describe the value y[] of a ivestmet by settig ρ=+r/00, where r is the iterest rate per period, expressed i percet. Fid the trasfer fuctio of this system ad determie whether it ca be both stable ad causal. <Sol.> The trasfer fuctio is determied by usig -trasform: H ( ) This LTI system caot be both stable ad causal, because the pole at = ρ > 38

39 Iverse System Give a LTI system with impulse respose h[], the impulse respose of the iverse system, h iv [], satisfies the coditio h iv * h H iv ( ) H ( ) or H iv ( ) H ( ) the poles of the iverse system H iv () are the eros of H(), ad vice versa a stable ad causal iverse system exists oly if all of the eros of H() are iside the uit circle i the -plae. A (stable ad causal) H() has all of its poles ad eros iside the uit circle H() is miimum phase. 39 A omiimum-phase system caot have a stable ad causal iverse system.

40 Example A LTI system is described by the differece equatio Fid the trasfer fuctio of the iverse system. Does a stable ad causal LTI iverse system exist? ] [ 8 ] [ 4 ] [ 4 ] [ x x x y y y <Sol.> The trasfer fuctio of the give system is ) ( ) )( ( ) ( H Hece, the iverse system the has the trasfer fuctio Both of the poles of the iverse system, i.e. =/4 ad =/, are iside the uit circle. The iverse system ca be both stable ad causal. Note that this system is also miimum phase, sice all eros ad poles of the system are iside the uit circle. ) )( ( ) ( ) ( 4 H iv

41 Example 7.9 Recall a two-path commuicatio chael is described by y x[ ] ax[ ] Fid the trasfer fuctio ad differece-equatio descriptio of the iverse system. What must the parameter a satisfy for the iverse system to be stable ad causal? <Sol.> First fid the trasfer fuctio of the two-path multiple chael system: H ( ) a The, the trasfer fuctio of the iverse system is ( ) H ( ) a The correspodig differece-equatio represetatio is y H iv ay x The iverse system is both stable ad causal whe a <. 4

42 Outlie Itroductio The -Trasform Properties of the Regio of Covergece Properties of the -Trasform Iversio of the -Trasform The Trasfer Fuctio Causality ad Stability Determiig Frequecy Respose from Poles & Zeros Computatioal Structures for DT-LTI Systems The Uilateral -Trasform 4

The z-transform. 7.1 Introduction. 7.2 The z-transform Derivation of the z-transform: x[n] = z n LTI system, h[n] z = re j

The z-transform. 7.1 Introduction. 7.2 The z-transform Derivation of the z-transform: x[n] = z n LTI system, h[n] z = re j The -Trasform 7. Itroductio Geeralie the complex siusoidal represetatio offered by DTFT to a represetatio of complex expoetial sigals. Obtai more geeral characteristics for discrete-time LTI systems. 7.

More information

Chapter 7 z-transform

Chapter 7 z-transform Chapter 7 -Trasform Itroductio Trasform Uilateral Trasform Properties Uilateral Trasform Iversio of Uilateral Trasform Determiig the Frequecy Respose from Poles ad Zeros Itroductio Role i Discrete-Time

More information

The z transform is the discrete-time counterpart of the Laplace transform. Other description: see page 553, textbook.

The z transform is the discrete-time counterpart of the Laplace transform. Other description: see page 553, textbook. The -Trasform 7. Itroductio The trasform is the discrete-time couterpart of the Laplace trasform. Other descriptio: see page 553, textbook. 7. The -trasform Derivatio of the -trasform: x[] re jω LTI system,

More information

Definition of z-transform.

Definition of z-transform. - Trasforms Frequecy domai represetatios of discretetime sigals ad LTI discrete-time systems are made possible with the use of DTFT. However ot all discrete-time sigals e.g. uit step sequece are guarateed

More information

Generalizing the DTFT. The z Transform. Complex Exponential Excitation. The Transfer Function. Systems Described by Difference Equations

Generalizing the DTFT. The z Transform. Complex Exponential Excitation. The Transfer Function. Systems Described by Difference Equations Geeraliig the DTFT The Trasform M. J. Roberts - All Rights Reserved. Edited by Dr. Robert Akl 1 The forward DTFT is defied by X e jω = x e jω i which = Ω is discrete-time radia frequecy, a real variable.

More information

Chapter 3. z-transform

Chapter 3. z-transform Chapter 3 -Trasform 3.0 Itroductio The -Trasform has the same role as that played by the Laplace Trasform i the cotiuous-time theorem. It is a liear operator that is useful for aalyig LTI systems such

More information

3. Z Transform. Recall that the Fourier transform (FT) of a DT signal xn [ ] is ( ) [ ] = In order for the FT to exist in the finite magnitude sense,

3. Z Transform. Recall that the Fourier transform (FT) of a DT signal xn [ ] is ( ) [ ] = In order for the FT to exist in the finite magnitude sense, 3. Z Trasform Referece: Etire Chapter 3 of text. Recall that the Fourier trasform (FT) of a DT sigal x [ ] is ω ( ) [ ] X e = j jω k = xe I order for the FT to exist i the fiite magitude sese, S = x [

More information

Z - Transform. It offers the techniques for digital filter design and frequency analysis of digital signals.

Z - Transform. It offers the techniques for digital filter design and frequency analysis of digital signals. Z - Trasform The -trasform is a very importat tool i describig ad aalyig digital systems. It offers the techiques for digital filter desig ad frequecy aalysis of digital sigals. Defiitio of -trasform:

More information

M2.The Z-Transform and its Properties

M2.The Z-Transform and its Properties M2.The Z-Trasform ad its Properties Readig Material: Page 94-126 of chapter 3 3/22/2011 I. Discrete-Time Sigals ad Systems 1 What did we talk about i MM1? MM1 - Discrete-Time Sigal ad System 3/22/2011

More information

from definition we note that for sequences which are zero for n < 0, X[z] involves only negative powers of z.

from definition we note that for sequences which are zero for n < 0, X[z] involves only negative powers of z. We ote that for the past four examples we have expressed the -trasform both as a ratio of polyomials i ad as a ratio of polyomials i -. The questio is how does oe kow which oe to use? [] X ] from defiitio

More information

6.003 Homework #3 Solutions

6.003 Homework #3 Solutions 6.00 Homework # Solutios Problems. Complex umbers a. Evaluate the real ad imagiary parts of j j. π/ Real part = Imagiary part = 0 e Euler s formula says that j = e jπ/, so jπ/ j π/ j j = e = e. Thus the

More information

COMM 602: Digital Signal Processing

COMM 602: Digital Signal Processing COMM 60: Digital Sigal Processig Lecture 4 -Properties of LTIS Usig Z-Trasform -Iverse Z-Trasform Properties of LTIS Usig Z-Trasform Properties of LTIS Usig Z-Trasform -ve +ve Properties of LTIS Usig Z-Trasform

More information

Time-Domain Representations of LTI Systems

Time-Domain Representations of LTI Systems 2.1 Itroductio Objectives: 1. Impulse resposes of LTI systems 2. Liear costat-coefficiets differetial or differece equatios of LTI systems 3. Bloc diagram represetatios of LTI systems 4. State-variable

More information

Digital Signal Processing

Digital Signal Processing Digital Sigal Processig Z-trasform dftwave -Trasform Backgroud-Defiitio - Fourier trasform j ω j ω e x e extracts the essece of x but is limited i the sese that it ca hadle stable systems oly. jω e coverges

More information

Frequency Response of FIR Filters

Frequency Response of FIR Filters EEL335: Discrete-Time Sigals ad Systems. Itroductio I this set of otes, we itroduce the idea of the frequecy respose of LTI systems, ad focus specifically o the frequecy respose of FIR filters.. Steady-state

More information

The z Transform. The Discrete LTI System Response to a Complex Exponential

The z Transform. The Discrete LTI System Response to a Complex Exponential The Trasform The trasform geeralies the Discrete-time Forier Trasform for the etire complex plae. For the complex variable is sed the otatio: jω x+ j y r e ; x, y Ω arg r x + y {} The Discrete LTI System

More information

Chapter 4 : Laplace Transform

Chapter 4 : Laplace Transform 4. Itroductio Laplace trasform is a alterative to solve the differetial equatio by the complex frequecy domai ( s = σ + jω), istead of the usual time domai. The DE ca be easily trasformed ito a algebraic

More information

Module 18 Discrete Time Signals and Z-Transforms Objective: Introduction : Description: Discrete Time Signal representation

Module 18 Discrete Time Signals and Z-Transforms Objective: Introduction : Description: Discrete Time Signal representation Module 8 Discrete Time Sigals ad Z-Trasforms Objective:To uderstad represetig discrete time sigals, apply z trasform for aalyzigdiscrete time sigals ad to uderstad the relatio to Fourier trasform Itroductio

More information

Chapter 2 Systems and Signals

Chapter 2 Systems and Signals Chapter 2 Systems ad Sigals 1 Itroductio Discrete-Time Sigals: Sequeces Discrete-Time Systems Properties of Liear Time-Ivariat Systems Liear Costat-Coefficiet Differece Equatios Frequecy-Domai Represetatio

More information

The z-transform can be used to obtain compact transform-domain representations of signals and systems. It

The z-transform can be used to obtain compact transform-domain representations of signals and systems. It 3 4 5 6 7 8 9 10 CHAPTER 3 11 THE Z-TRANSFORM 31 INTRODUCTION The z-trasform ca be used to obtai compact trasform-domai represetatios of sigals ad systems It provides ituitio particularly i LTI system

More information

The Z-Transform. Content and Figures are from Discrete-Time Signal Processing, 2e by Oppenheim, Shafer, and Buck, Prentice Hall Inc.

The Z-Transform. Content and Figures are from Discrete-Time Signal Processing, 2e by Oppenheim, Shafer, and Buck, Prentice Hall Inc. The Z-Trasform Cotet ad Figures are from Discrete-Time Sigal Processig, e by Oppeheim, Shafer, ad Buck, 999- Pretice Hall Ic. The -Trasform Couterpart of the Laplace trasform for discrete-time sigals Geeraliatio

More information

Solutions of Chapter 5 Part 1/2

Solutions of Chapter 5 Part 1/2 Page 1 of 8 Solutios of Chapter 5 Part 1/2 Problem 5.1-1 Usig the defiitio, compute the -trasform of x[] ( 1) (u[] u[ 8]). Sketch the poles ad eros of X[] i the plae. Solutio: Accordig to the defiitio,

More information

The Z-Transform. (t-t 0 ) Figure 1: Simplified graph of an impulse function. For an impulse, it can be shown that (1)

The Z-Transform. (t-t 0 ) Figure 1: Simplified graph of an impulse function. For an impulse, it can be shown that (1) The Z-Trasform Sampled Data The geeralied fuctio (t) (also kow as the impulse fuctio) is useful i the defiitio ad aalysis of sampled-data sigals. Figure below shows a simplified graph of a impulse. (t-t

More information

Lecture 3. Digital Signal Processing. Chapter 3. z-transforms. Mikael Swartling Nedelko Grbic Bengt Mandersson. rev. 2016

Lecture 3. Digital Signal Processing. Chapter 3. z-transforms. Mikael Swartling Nedelko Grbic Bengt Mandersson. rev. 2016 Lecture 3 Digital Sigal Processig Chapter 3 z-trasforms Mikael Swartlig Nedelko Grbic Begt Madersso rev. 06 Departmet of Electrical ad Iformatio Techology Lud Uiversity z-trasforms We defie the z-trasform

More information

Ch3 Discrete Time Fourier Transform

Ch3 Discrete Time Fourier Transform Ch3 Discrete Time Fourier Trasform 3. Show that the DTFT of [] is give by ( k). e k 3. Determie the DTFT of the two sided sigal y [ ],. 3.3 Determie the DTFT of the causal sequece x[ ] A cos( 0 ) [ ],

More information

Question1 Multiple choices (circle the most appropriate one):

Question1 Multiple choices (circle the most appropriate one): Philadelphia Uiversity Studet Name: Faculty of Egieerig Studet Number: Dept. of Computer Egieerig Fial Exam, First Semester: 2014/2015 Course Title: Digital Sigal Aalysis ad Processig Date: 01/02/2015

More information

Solutions. Number of Problems: 4. None. Use only the prepared sheets for your solutions. Additional paper is available from the supervisors.

Solutions. Number of Problems: 4. None. Use only the prepared sheets for your solutions. Additional paper is available from the supervisors. Quiz November 4th, 23 Sigals & Systems (5-575-) P. Reist & Prof. R. D Adrea Solutios Exam Duratio: 4 miutes Number of Problems: 4 Permitted aids: Noe. Use oly the prepared sheets for your solutios. Additioal

More information

ECE-S352 Introduction to Digital Signal Processing Lecture 3A Direct Solution of Difference Equations

ECE-S352 Introduction to Digital Signal Processing Lecture 3A Direct Solution of Difference Equations ECE-S352 Itroductio to Digital Sigal Processig Lecture 3A Direct Solutio of Differece Equatios Discrete Time Systems Described by Differece Equatios Uit impulse (sample) respose h() of a DT system allows

More information

Appendix: The Laplace Transform

Appendix: The Laplace Transform Appedix: The Laplace Trasform The Laplace trasform is a powerful method that ca be used to solve differetial equatio, ad other mathematical problems. Its stregth lies i the fact that it allows the trasformatio

More information

EE / EEE SAMPLE STUDY MATERIAL. GATE, IES & PSUs Signal System. Electrical Engineering. Postal Correspondence Course

EE / EEE SAMPLE STUDY MATERIAL. GATE, IES & PSUs Signal System. Electrical Engineering. Postal Correspondence Course Sigal-EE Postal Correspodece Course 1 SAMPLE STUDY MATERIAL Electrical Egieerig EE / EEE Postal Correspodece Course GATE, IES & PSUs Sigal System Sigal-EE Postal Correspodece Course CONTENTS 1. SIGNAL

More information

Lesson 10: Limits and Continuity

Lesson 10: Limits and Continuity www.scimsacademy.com Lesso 10: Limits ad Cotiuity SCIMS Academy 1 Limit of a fuctio The cocept of limit of a fuctio is cetral to all other cocepts i calculus (like cotiuity, derivative, defiite itegrals

More information

FIR Filter Design: Part II

FIR Filter Design: Part II EEL335: Discrete-Time Sigals ad Systems. Itroductio I this set of otes, we cosider how we might go about desigig FIR filters with arbitrary frequecy resposes, through compositio of multiple sigle-peak

More information

Web Appendix O - Derivations of the Properties of the z Transform

Web Appendix O - Derivations of the Properties of the z Transform M. J. Roberts - 2/18/07 Web Appedix O - Derivatios of the Properties of the z Trasform O.1 Liearity Let z = x + y where ad are costats. The ( z)= ( x + y )z = x z + y z ad the liearity property is O.2

More information

CEMTool Tutorial. The z-transform

CEMTool Tutorial. The z-transform CEMTool Tutorial The -Trasform 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

GATE ELECTRONICS & COMMUNICATION

GATE ELECTRONICS & COMMUNICATION Eighth Editio GATE ELECTRONICS & COMMUNICATION Sigals ad Systems Vol 7 of 0 RK Kaodia Ashish Murolia NODIA & COMPANY GATE Electroics & Commuicatio Vol 7, 8e Sigals ad Systems RK Kaodia & Ashish Murolia

More information

Module 2: z-transform and Discrete Systems

Module 2: z-transform and Discrete Systems Module : -Trasform ad Discrete Systems Prof. Eliathamy Amikairajah ajah Dr. Tharmarajah Thiruvara School of Electrical Egieerig & Telecommuicatios The Uiversity of New South Wales Australia The -Trasform

More information

Exponential Moving Average Pieter P

Exponential Moving Average Pieter P Expoetial Movig Average Pieter P Differece equatio The Differece equatio of a expoetial movig average lter is very simple: y[] x[] + (1 )y[ 1] I this equatio, y[] is the curret output, y[ 1] is the previous

More information

University of California at Berkeley College of Engineering Department of Electrical Engineering and Computer Sciences

University of California at Berkeley College of Engineering Department of Electrical Engineering and Computer Sciences A Uiversity of Califoria at Berkeley College of Egieerig Departmet of Electrical Egieerig ad Computer Scieces U N I V E R S T H E I T Y O F LE T TH E R E B E LI G H T C A L I F O R N 8 6 8 I A EECS : Sigals

More information

Discrete-Time Systems, LTI Systems, and Discrete-Time Convolution

Discrete-Time Systems, LTI Systems, and Discrete-Time Convolution EEL5: Discrete-Time Sigals ad Systems. Itroductio I this set of otes, we begi our mathematical treatmet of discrete-time s. As show i Figure, a discrete-time operates or trasforms some iput sequece x [

More information

Dynamic Response of Linear Systems

Dynamic Response of Linear Systems Dyamic Respose of Liear Systems Liear System Respose Superpositio Priciple Resposes to Specific Iputs Dyamic Respose of st Order Systems Characteristic Equatio - Free Respose Stable st Order System Respose

More information

Practical Spectral Anaysis (continue) (from Boaz Porat s book) Frequency Measurement

Practical Spectral Anaysis (continue) (from Boaz Porat s book) Frequency Measurement Practical Spectral Aaysis (cotiue) (from Boaz Porat s book) Frequecy Measuremet Oe of the most importat applicatios of the DFT is the measuremet of frequecies of periodic sigals (eg., siusoidal sigals),

More information

Signal Processing in Mechatronics. Lecture 3, Convolution, Fourier Series and Fourier Transform

Signal Processing in Mechatronics. Lecture 3, Convolution, Fourier Series and Fourier Transform Sigal Processig i Mechatroics Summer semester, 1 Lecture 3, Covolutio, Fourier Series ad Fourier rasform Dr. Zhu K.P. AIS, UM 1 1. Covolutio Covolutio Descriptio of LI Systems he mai premise is that the

More information

EE Midterm Test 1 - Solutions

EE Midterm Test 1 - Solutions EE35 - Midterm Test - Solutios Total Poits: 5+ 6 Bous Poits Time: hour. ( poits) Cosider the parallel itercoectio of the two causal systems, System ad System 2, show below. System x[] + y[] System 2 The

More information

ADVANCED DIGITAL SIGNAL PROCESSING

ADVANCED DIGITAL SIGNAL PROCESSING ADVANCED DIGITAL SIGNAL PROCESSING PROF. S. C. CHAN (email : sccha@eee.hku.hk, Rm. CYC-702) DISCRETE-TIME SIGNALS AND SYSTEMS MULTI-DIMENSIONAL SIGNALS AND SYSTEMS RANDOM PROCESSES AND APPLICATIONS ADAPTIVE

More information

Analog and Digital Signals. Introduction to Digital Signal Processing. Discrete-time Sinusoids. Analog and Digital Signals

Analog and Digital Signals. Introduction to Digital Signal Processing. Discrete-time Sinusoids. Analog and Digital Signals Itroductio to Digital Sigal Processig Chapter : Itroductio Aalog ad Digital Sigals aalog = cotiuous-time cotiuous amplitude digital = discrete-time discrete amplitude cotiuous amplitude discrete amplitude

More information

We are mainly going to be concerned with power series in x, such as. (x)} converges - that is, lims N n

We are mainly going to be concerned with power series in x, such as. (x)} converges - that is, lims N n Review of Power Series, Power Series Solutios A power series i x - a is a ifiite series of the form c (x a) =c +c (x a)+(x a) +... We also call this a power series cetered at a. Ex. (x+) is cetered at

More information

Digital signal processing: Lecture 5. z-transformation - I. Produced by Qiangfu Zhao (Since 1995), All rights reserved

Digital signal processing: Lecture 5. z-transformation - I. Produced by Qiangfu Zhao (Since 1995), All rights reserved Digital sigal processig: Lecture 5 -trasformatio - I Produced by Qiagfu Zhao Sice 995, All rights reserved DSP-Lec5/ Review of last lecture Fourier trasform & iverse Fourier trasform: Time domai & Frequecy

More information

Quiz. Use either the RATIO or ROOT TEST to determine whether the series is convergent or not.

Quiz. Use either the RATIO or ROOT TEST to determine whether the series is convergent or not. Quiz. Use either the RATIO or ROOT TEST to determie whether the series is coverget or ot. e .6 POWER SERIES Defiitio. A power series i about is a series of the form c 0 c a c a... c a... a 0 c a where

More information

Complex Numbers Solutions

Complex Numbers Solutions Complex Numbers Solutios Joseph Zoller February 7, 06 Solutios. (009 AIME I Problem ) There is a complex umber with imagiary part 64 ad a positive iteger such that Fid. [Solutio: 697] 4i + + 4i. 4i 4i

More information

EECE 301 Signals & Systems

EECE 301 Signals & Systems EECE 301 Sigals & Systems Prof. Mark Fowler Note Set #8 D-T Covolutio: The Tool for Fidig the Zero-State Respose Readig Assigmet: Sectio 2.1-2.2 of Kame ad Heck 1/14 Course Flow Diagram The arrows here

More information

TEACHER CERTIFICATION STUDY GUIDE

TEACHER CERTIFICATION STUDY GUIDE COMPETENCY 1. ALGEBRA SKILL 1.1 1.1a. ALGEBRAIC STRUCTURES Kow why the real ad complex umbers are each a field, ad that particular rigs are ot fields (e.g., itegers, polyomial rigs, matrix rigs) Algebra

More information

CHAPTER 10 INFINITE SEQUENCES AND SERIES

CHAPTER 10 INFINITE SEQUENCES AND SERIES CHAPTER 10 INFINITE SEQUENCES AND SERIES 10.1 Sequeces 10.2 Ifiite Series 10.3 The Itegral Tests 10.4 Compariso Tests 10.5 The Ratio ad Root Tests 10.6 Alteratig Series: Absolute ad Coditioal Covergece

More information

SOLUTIONS TO EXAM 3. Solution: Note that this defines two convergent geometric series with respective radii r 1 = 2/5 < 1 and r 2 = 1/5 < 1.

SOLUTIONS TO EXAM 3. Solution: Note that this defines two convergent geometric series with respective radii r 1 = 2/5 < 1 and r 2 = 1/5 < 1. SOLUTIONS TO EXAM 3 Problem Fid the sum of the followig series 2 + ( ) 5 5 2 5 3 25 2 2 This series diverges Solutio: Note that this defies two coverget geometric series with respective radii r 2/5 < ad

More information

Olli Simula T / Chapter 1 3. Olli Simula T / Chapter 1 5

Olli Simula T / Chapter 1 3. Olli Simula T / Chapter 1 5 Sigals ad Systems Sigals ad Systems Sigals are variables that carry iformatio Systemstake sigals as iputs ad produce sigals as outputs The course deals with the passage of sigals through systems T-6.4

More information

ENGI Series Page 6-01

ENGI Series Page 6-01 ENGI 3425 6 Series Page 6-01 6. Series Cotets: 6.01 Sequeces; geeral term, limits, covergece 6.02 Series; summatio otatio, covergece, divergece test 6.03 Stadard Series; telescopig series, geometric series,

More information

APPENDIX F Complex Numbers

APPENDIX F Complex Numbers APPENDIX F Complex Numbers Operatios with Complex Numbers Complex Solutios of Quadratic Equatios Polar Form of a Complex Number Powers ad Roots of Complex Numbers Operatios with Complex Numbers Some equatios

More information

Course Outline. Designing Control Systems. Proportional Controller. Amme 3500 : System Dynamics and Control. Root Locus. Dr. Stefan B.

Course Outline. Designing Control Systems. Proportional Controller. Amme 3500 : System Dynamics and Control. Root Locus. Dr. Stefan B. Amme 3500 : System Dyamics ad Cotrol Root Locus Course Outlie Week Date Cotet Assigmet Notes Mar Itroductio 8 Mar Frequecy Domai Modellig 3 5 Mar Trasiet Performace ad the s-plae 4 Mar Block Diagrams Assig

More information

MIDTERM 3 CALCULUS 2. Monday, December 3, :15 PM to 6:45 PM. Name PRACTICE EXAM SOLUTIONS

MIDTERM 3 CALCULUS 2. Monday, December 3, :15 PM to 6:45 PM. Name PRACTICE EXAM SOLUTIONS MIDTERM 3 CALCULUS MATH 300 FALL 08 Moday, December 3, 08 5:5 PM to 6:45 PM Name PRACTICE EXAM S Please aswer all of the questios, ad show your work. You must explai your aswers to get credit. You will

More information

2D DSP Basics: 2D Systems

2D DSP Basics: 2D Systems - Digital Image Processig ad Compressio D DSP Basics: D Systems D Systems T[ ] y = T [ ] Liearity Additivity: If T y = T [ ] The + T y = y + y Homogeeity: If The T y = T [ ] a T y = ay = at [ ] Liearity

More information

Signals and Systems. Problem Set: From Continuous-Time to Discrete-Time

Signals and Systems. Problem Set: From Continuous-Time to Discrete-Time Sigals ad Systems Problem Set: From Cotiuous-Time to Discrete-Time Updated: October 5, 2017 Problem Set Problem 1 - Liearity ad Time-Ivariace Cosider the followig systems ad determie whether liearity ad

More information

62. Power series Definition 16. (Power series) Given a sequence {c n }, the series. c n x n = c 0 + c 1 x + c 2 x 2 + c 3 x 3 +

62. Power series Definition 16. (Power series) Given a sequence {c n }, the series. c n x n = c 0 + c 1 x + c 2 x 2 + c 3 x 3 + 62. Power series Defiitio 16. (Power series) Give a sequece {c }, the series c x = c 0 + c 1 x + c 2 x 2 + c 3 x 3 + is called a power series i the variable x. The umbers c are called the coefficiets of

More information

Signal Processing. Lecture 02: Discrete Time Signals and Systems. Ahmet Taha Koru, Ph. D. Yildiz Technical University.

Signal Processing. Lecture 02: Discrete Time Signals and Systems. Ahmet Taha Koru, Ph. D. Yildiz Technical University. Sigal Processig Lecture 02: Discrete Time Sigals ad Systems Ahmet Taha Koru, Ph. D. Yildiz Techical Uiversity 2017-2018 Fall ATK (YTU) Sigal Processig 2017-2018 Fall 1 / 51 Discrete Time Sigals Discrete

More information

Chapter 8. DFT : The Discrete Fourier Transform

Chapter 8. DFT : The Discrete Fourier Transform Chapter 8 DFT : The Discrete Fourier Trasform Roots of Uity Defiitio: A th root of uity is a complex umber x such that x The th roots of uity are: ω, ω,, ω - where ω e π /. Proof: (ω ) (e π / ) (e π )

More information

CALCULUS BASIC SUMMER REVIEW

CALCULUS BASIC SUMMER REVIEW CALCULUS BASIC SUMMER REVIEW NAME rise y y y Slope of a o vertical lie: m ru Poit Slope Equatio: y y m( ) The slope is m ad a poit o your lie is, ). ( y Slope-Itercept Equatio: y m b slope= m y-itercept=

More information

Signals & Systems Chapter3

Signals & Systems Chapter3 Sigals & Systems Chapter3 1.2 Discrete-Time (D-T) Sigals Electroic systems do most of the processig of a sigal usig a computer. A computer ca t directly process a C-T sigal but istead eeds a stream of

More information

1the 1it is said to be overdamped. When 1, the roots of

1the 1it is said to be overdamped. When 1, the roots of Homework 3 AERE573 Fall 08 Due 0/8(M) ame PROBLEM (40pts) Cosider a D order uderdamped system trasfer fuctio H( s) s ratio 0 The deomiator is the system characteristic polyomial P( s) s s (a)(5pts) Use

More information

ELEG 4603/5173L Digital Signal Processing Ch. 1 Discrete-Time Signals and Systems

ELEG 4603/5173L Digital Signal Processing Ch. 1 Discrete-Time Signals and Systems Departmet of Electrical Egieerig Uiversity of Arasas ELEG 4603/5173L Digital Sigal Processig Ch. 1 Discrete-Time Sigals ad Systems Dr. Jigxia Wu wuj@uar.edu OUTLINE 2 Classificatios of discrete-time sigals

More information

Introduction to Signals and Systems, Part V: Lecture Summary

Introduction to Signals and Systems, Part V: Lecture Summary EEL33: Discrete-Time Sigals ad Systems Itroductio to Sigals ad Systems, Part V: Lecture Summary Itroductio to Sigals ad Systems, Part V: Lecture Summary So far we have oly looked at examples of o-recursive

More information

x[0] x[1] x[2] Figure 2.1 Graphical representation of a discrete-time signal.

x[0] x[1] x[2] Figure 2.1 Graphical representation of a discrete-time signal. x[ ] x[ ] x[] x[] x[] x[] 9 8 7 6 5 4 3 3 4 5 6 7 8 9 Figure. Graphical represetatio of a discrete-time sigal. From Discrete-Time Sigal Processig, e by Oppeheim, Schafer, ad Buck 999- Pretice Hall, Ic.

More information

Chapter 4. Fourier Series

Chapter 4. Fourier Series Chapter 4. Fourier Series At this poit we are ready to ow cosider the caoical equatios. Cosider, for eample the heat equatio u t = u, < (4.) subject to u(, ) = si, u(, t) = u(, t) =. (4.) Here,

More information

Chapter 10: Power Series

Chapter 10: Power Series Chapter : Power Series 57 Chapter Overview: Power Series The reaso series are part of a Calculus course is that there are fuctios which caot be itegrated. All power series, though, ca be itegrated because

More information

Appendix F: Complex Numbers

Appendix F: Complex Numbers Appedix F Complex Numbers F1 Appedix F: Complex Numbers Use the imagiary uit i to write complex umbers, ad to add, subtract, ad multiply complex umbers. Fid complex solutios of quadratic equatios. Write

More information

Discrete-Time Signals and Systems. Signals and Systems. Digital Signals. Discrete-Time Signals. Operations on Sequences: Basic Operations

Discrete-Time Signals and Systems. Signals and Systems. Digital Signals. Discrete-Time Signals. Operations on Sequences: Basic Operations -6.3 Digital Sigal Processig ad Filterig..8 Discrete-ime Sigals ad Systems ime-domai Represetatios of Discrete-ime Sigals ad Systems ime-domai represetatio of a discrete-time sigal as a sequece of umbers

More information

MAT 271 Project: Partial Fractions for certain rational functions

MAT 271 Project: Partial Fractions for certain rational functions MAT 7 Project: Partial Fractios for certai ratioal fuctios Prerequisite kowledge: partial fractios from MAT 7, a very good commad of factorig ad complex umbers from Precalculus. To complete this project,

More information

PRELIM PROBLEM SOLUTIONS

PRELIM PROBLEM SOLUTIONS PRELIM PROBLEM SOLUTIONS THE GRAD STUDENTS + KEN Cotets. Complex Aalysis Practice Problems 2. 2. Real Aalysis Practice Problems 2. 4 3. Algebra Practice Problems 2. 8. Complex Aalysis Practice Problems

More information

Fall 2011, EE123 Digital Signal Processing

Fall 2011, EE123 Digital Signal Processing Lecture 5 Miki Lustig, UCB September 14, 211 Miki Lustig, UCB Motivatios for Discrete Fourier Trasform Sampled represetatio i time ad frequecy umerical Fourier aalysis requires a Fourier represetatio that

More information

Frequency Domain Filtering

Frequency Domain Filtering Frequecy Domai Filterig Raga Rodrigo October 19, 2010 Outlie Cotets 1 Itroductio 1 2 Fourier Represetatio of Fiite-Duratio Sequeces: The Discrete Fourier Trasform 1 3 The 2-D Discrete Fourier Trasform

More information

CHAPTER 1 SEQUENCES AND INFINITE SERIES

CHAPTER 1 SEQUENCES AND INFINITE SERIES CHAPTER SEQUENCES AND INFINITE SERIES SEQUENCES AND INFINITE SERIES (0 meetigs) Sequeces ad limit of a sequece Mootoic ad bouded sequece Ifiite series of costat terms Ifiite series of positive terms Alteratig

More information

Exam. Notes: A single A4 sheet of paper (double sided; hand-written or computer typed)

Exam. Notes: A single A4 sheet of paper (double sided; hand-written or computer typed) Exam February 8th, 8 Sigals & Systems (5-575-) Prof. R. D Adrea Exam Exam Duratio: 5 Mi Number of Problems: 5 Number of Poits: 5 Permitted aids: Importat: Notes: A sigle A sheet of paper (double sided;

More information

Ma 530 Introduction to Power Series

Ma 530 Introduction to Power Series Ma 530 Itroductio to Power Series Please ote that there is material o power series at Visual Calculus. Some of this material was used as part of the presetatio of the topics that follow. What is a Power

More information

ECE4270 Fundamentals of DSP. Lecture 2 Discrete-Time Signals and Systems & Difference Equations. Overview of Lecture 2. More Discrete-Time Systems

ECE4270 Fundamentals of DSP. Lecture 2 Discrete-Time Signals and Systems & Difference Equations. Overview of Lecture 2. More Discrete-Time Systems ECE4270 Fudametals of DSP Lecture 2 Discrete-Time Sigals ad Systems & Differece Equatios School of ECE Ceter for Sigal ad Iformatio Processig Georgia Istitute of Techology Overview of Lecture 2 Aoucemet

More information

6.003: Signals and Systems. Feedback, Poles, and Fundamental Modes

6.003: Signals and Systems. Feedback, Poles, and Fundamental Modes 6.003: Sigals ad Systems Feedback, Poles, ad Fudametal Modes February 9, 2010 Last Time: Multiple Represetatios of DT Systems Verbal descriptios: preserve the ratioale. To reduce the umber of bits eeded

More information

DIGITAL SIGNAL PROCESSING LECTURE 3

DIGITAL SIGNAL PROCESSING LECTURE 3 DIGITAL SIGNAL PROCESSING LECTURE 3 Fall 2 2K8-5 th Semester Tahir Muhammad tmuhammad_7@yahoo.com Cotet ad Figures are from Discrete-Time Sigal Processig, 2e by Oppeheim, Shafer, ad Buc, 999-2 Pretice

More information

: Transforms and Partial Differential Equations

: Transforms and Partial Differential Equations Trasforms ad Partial Differetial Equatios 018 SUBJECT NAME : Trasforms ad Partial Differetial Equatios SUBJECT CODE : MA 6351 MATERIAL NAME : Part A questios REGULATION : R013 WEBSITE : wwwharigaeshcom

More information

Lecture 4 Conformal Mapping and Green s Theorem. 1. Let s try to solve the following problem by separation of variables

Lecture 4 Conformal Mapping and Green s Theorem. 1. Let s try to solve the following problem by separation of variables Lecture 4 Coformal Mappig ad Gree s Theorem Today s topics. Solvig electrostatic problems cotiued. Why separatio of variables does t always work 3. Coformal mappig 4. Gree s theorem The failure of separatio

More information

Apply change-of-basis formula to rewrite x as a linear combination of eigenvectors v j.

Apply change-of-basis formula to rewrite x as a linear combination of eigenvectors v j. Eigevalue-Eigevector Istructor: Nam Su Wag eigemcd Ay vector i real Euclidea space of dimesio ca be uiquely epressed as a liear combiatio of liearly idepedet vectors (ie, basis) g j, j,,, α g α g α g α

More information

f(x) dx as we do. 2x dx x also diverges. Solution: We compute 2x dx lim

f(x) dx as we do. 2x dx x also diverges. Solution: We compute 2x dx lim Math 3, Sectio 2. (25 poits) Why we defie f(x) dx as we do. (a) Show that the improper itegral diverges. Hece the improper itegral x 2 + x 2 + b also diverges. Solutio: We compute x 2 + = lim b x 2 + =

More information

Beurling Integers: Part 2

Beurling Integers: Part 2 Beurlig Itegers: Part 2 Isomorphisms Devi Platt July 11, 2015 1 Prime Factorizatio Sequeces I the last article we itroduced the Beurlig geeralized itegers, which ca be represeted as a sequece of real umbers

More information

Q-BINOMIALS AND THE GREATEST COMMON DIVISOR. Keith R. Slavin 8474 SW Chevy Place, Beaverton, Oregon 97008, USA.

Q-BINOMIALS AND THE GREATEST COMMON DIVISOR. Keith R. Slavin 8474 SW Chevy Place, Beaverton, Oregon 97008, USA. INTEGERS: ELECTRONIC JOURNAL OF COMBINATORIAL NUMBER THEORY 8 2008, #A05 Q-BINOMIALS AND THE GREATEST COMMON DIVISOR Keith R. Slavi 8474 SW Chevy Place, Beaverto, Orego 97008, USA slavi@dsl-oly.et Received:

More information

( ) ( ) ( ) ( ) ( + ) ( )

( ) ( ) ( ) ( ) ( + ) ( ) LSM Nov. 00 Cotet List Mathematics (AH). Algebra... kow ad use the otatio!, C r ad r.. kow the results = r r + + = r r r..3 kow Pascal's triagle. Pascal's triagle should be eteded up to = 7...4 kow ad

More information

Chapter 6 Infinite Series

Chapter 6 Infinite Series Chapter 6 Ifiite Series I the previous chapter we cosidered itegrals which were improper i the sese that the iterval of itegratio was ubouded. I this chapter we are goig to discuss a topic which is somewhat

More information

Mechatronics. Time Response & Frequency Response 2 nd -Order Dynamic System 2-Pole, Low-Pass, Active Filter

Mechatronics. Time Response & Frequency Response 2 nd -Order Dynamic System 2-Pole, Low-Pass, Active Filter Time Respose & Frequecy Respose d -Order Dyamic System -Pole, Low-Pass, Active Filter R 4 R 7 C 5 e i R 1 C R 3 - + R 6 - + e out Assigmet: Perform a Complete Dyamic System Ivestigatio of the Two-Pole,

More information

Infinite Sequences and Series

Infinite Sequences and Series Chapter 6 Ifiite Sequeces ad Series 6.1 Ifiite Sequeces 6.1.1 Elemetary Cocepts Simply speakig, a sequece is a ordered list of umbers writte: {a 1, a 2, a 3,...a, a +1,...} where the elemets a i represet

More information

AP Calculus Chapter 9: Infinite Series

AP Calculus Chapter 9: Infinite Series AP Calculus Chapter 9: Ifiite Series 9. Sequeces a, a 2, a 3, a 4, a 5,... Sequece: A fuctio whose domai is the set of positive itegers = 2 3 4 a = a a 2 a 3 a 4 terms of the sequece Begi with the patter

More information

Finite-length Discrete Transforms. Chapter 5, Sections

Finite-length Discrete Transforms. Chapter 5, Sections Fiite-legth Discrete Trasforms Chapter 5, Sectios 5.2-50 5.0 Dr. Iyad djafar Outlie The Discrete Fourier Trasform (DFT) Matrix Represetatio of DFT Fiite-legth Sequeces Circular Covolutio DFT Symmetry Properties

More information

Frequency-domain Characteristics of Discrete-time LTI Systems

Frequency-domain Characteristics of Discrete-time LTI Systems requecy-domi Chrcteristics of Discrete-time LTI Systems Prof. Siripog Potisuk LTI System descriptio Previous bsis fuctio: uit smple or DT impulse The iput sequece is represeted s lier combitio of shifted

More information

CHAPTER NINE. Frequency Response Methods

CHAPTER NINE. Frequency Response Methods CHAPTER NINE 9. Itroductio It as poited earlier that i practice the performace of a feedback cotrol system is more preferably measured by its time - domai respose characteristics. This is i cotrast to

More information

G r a d e 1 1 P r e - C a l c u l u s M a t h e m a t i c s ( 3 0 S )

G r a d e 1 1 P r e - C a l c u l u s M a t h e m a t i c s ( 3 0 S ) G r a d e 1 1 P r e - C a l c u l u s M a t h e m a t i c s ( 3 0 S ) Grade 11 Pre-Calculus Mathematics (30S) is desiged for studets who ited to study calculus ad related mathematics as part of post-secodary

More information

1 1 2 = show that: over variables x and y. [2 marks] Write down necessary conditions involving first and second-order partial derivatives for ( x0, y

1 1 2 = show that: over variables x and y. [2 marks] Write down necessary conditions involving first and second-order partial derivatives for ( x0, y Questio (a) A square matrix A= A is called positive defiite if the quadratic form waw > 0 for every o-zero vector w [Note: Here (.) deotes the traspose of a matrix or a vector]. Let 0 A = 0 = show that:

More information

FFTs in Graphics and Vision. The Fast Fourier Transform

FFTs in Graphics and Vision. The Fast Fourier Transform FFTs i Graphics ad Visio The Fast Fourier Trasform 1 Outlie The FFT Algorithm Applicatios i 1D Multi-Dimesioal FFTs More Applicatios Real FFTs 2 Computatioal Complexity To compute the movig dot-product

More information