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082-Engineering-Mathematics-Anthony-Croft-Robert-Davison-Martin-Hargreaves-James-Flint-Edisi-5-2017

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706 Chapter 22 Difference equations and the z transform

22.9.1 Mappingthesplanetothezplane

When designing an engineering system it is often useful to consider ansplane representationofthesystem.Thecharacteristicsofasystemcanbequicklyidentifiedbythe

positionsofthepolesandzerosaswesawinChapter21.Engineerswilloftenmodifythe

system characteristics by introducing new poles and zeros or by changing the positions

ofexistingones.Unfortunately,itisnotconvenienttousethesplanetoanalysediscrete

systems. For a sampled signalEquation (22.9) yields

∞∑

F ∗ (s)=L{f ∗ (t)} = f[k]e −skT

k=0

ThecontinuoussignalsandsystemsthatwereanalysedinChapter21hadLaplacetransformsthatweresimpleratiosofpolynomials

ins.Thiswasoneofthemainreasonsfor

usingLaplacetransformstosolvedifferentialequations;theproblemwasreducedtoone

ofreasonablystraightforwardalgebraicmanipulation.HerewehaveaLaplacetransform

thatisverycomplicated.Infactitcanhaveaninfinitenumberofpolesandzeros.Tosee

this consider the following example.

( ) πt

Example22.16 The continuous signal f (t) = cos is sampled at 1 second intervals starting from

2

t=0.

(a) Find the Laplace transformof the sampled signal f ∗ (t).

(b) Show thatF ∗ (s)has an infinity of poles.

(c) Find theztransformof the sampled signaland show thatthis has justtwo poles.

( ) πt

Solution (a) The continuous signal f (t) = cos sampled at 1 second intervals gives rise to

2

the sequence 1,0, −1,0,1,0, −1,.... Consequently, fromEquation (22.9)

∞∑

∞∑

F ∗ (s)=L{f ∗ (t)} = f[k]e −skT = f[k]e −sk sinceT = 1

thatis,

k=0

k=0

F ∗ (s)=1+0−e −2s +0+e −4s +0−e −6s +···

This is a geometric progression with common ratio −e −2s and hence its sum to

infinity is

thatis,

1

1 − (−e −2s )

F ∗ 1

(s) =

1 +e −2s

(b) PolesofF ∗ (s)willoccurwhen1 +e −2s = 0.Writings = σ +jω weseethatpoles

will occur when e −2(σ+jω) = −1. Since −1 can be written as e j(2n−1)π ,n ∈ Z (see

Chapter 9), wesee thatpoles will occur when

e −2σ−2jω = e j(2n−1)π

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