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Summary
This document provides a detailed explanation of the Z-transform, focusing on the direct and inverse transforms, along with the region of convergence (ROC). It covers various aspects of the theory, including complex variable manipulation and practical examples.
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Z-Transform The Direct π-Transform The π-transform of a discrete-time signal π₯ power series is defined as the β π = ΰ· π₯ π=ββ π§βπ where π§ is a complex variable. The relation above is sometimes called transform. because it transforms the time- domain signal π₯ into its complex-plane representation π. T...
Z-Transform The Direct π-Transform The π-transform of a discrete-time signal π₯ power series is defined as the β π = ΰ· π₯ π=ββ π§βπ where π§ is a complex variable. The relation above is sometimes called transform. because it transforms the time- domain signal π₯ into its complex-plane representation π. The inverse procedure [i.e., obtaining π₯ inverse π-transform. the direct π- from π ] is called the The Direct π-Transform For convenience, the π-transform of a signal π₯is denoted by π β‘π whereas the relationship between π₯ π§ and π is indicated by π₯ π Since the π§-transform is an infinite power series, it exists only for those values of π§ for which this series converges. The region of convergence (ROC) of π π is the set of all values of π§ for which attains a finite value. Thus, any time we cite a π-transform we should also indicate its ROC. Radius of Convergence in Complex Plane Let us express the complex variable z in polar form as π§ = ππππ Where π = |π§| and πβ‘π§. Then π β can be expressed as, β = ΰ· π§βπ = ΰ· π₯ π π=ββ π=ββ βπ In the ROC of π π ,π = ΰ· π=ββ < β. So π₯ β βπ = π=ββ ΰ· π₯ π₯ πβπ Hence π is finite if the sequence π₯ πβπ is absolutely summable. Radius of Convergence in Complex Plane β π =ΰ·π₯ π=1 β ππ +ΰ·π₯ π=0 πβπ If π converges in some region of the complex plane, both summations in the equation above must be finite in that region. If the first sum converges, there must exist values of r small enough such that the product sequence π₯ absolutely summable. ππ , 1 π1, there is no common region of convergence for the two sums and hence X(z) does not exist. π-Transform Issue The previous examples raises an important issue regarding the uniqueness of the z-transform. Again, from the previous examples, the causal signal πΌππ’ and its anti-causal signal βπΌππ’ have identical closed-form expressions for the z-transform, that is, π =π 1 = 1 β πΌπ§β1 This implies that a closed-form expression for the z-transform does not uniquely specify the signal in the time domain. π-Transform Issue The ambiguity can be resolved only if in addition to the closed-form expression, the ROC is specified. In summary, a discrete-time signal π₯ is uniquely determined by its z-transform π and the region of convergence of π. Moving forward, the term βz-transformβ is used to refer to both the closed- form expression and the corresponding ROC. The previous examples also illustrates the point that the ROC of a causal signal is the exterior of a circle of some radius π2 while the ROC of an anti-causal signal is the interior of a circle of some radius π1. Example In determining the convergence of π , we consider two different cases: Case 1: π < πΌ In this case the two ROC above do not overlap. Consequently, we cannot find values of z for which both power series converge simultaneously. Clearly, in this case, X(z) does not exist. Example In determining convergence of the π , we consider two different cases: Case 2: π > πΌ In this case there is a ring in the z-plane where both power series converge (overlapping area). simultaneously, as shown in the figure. Example So if Case 2 is true, that is, π > πΌ , then π = 1 1 β πΌπ§β1 β 1 1 β ππ§β1 π = πβπΌ πΌ + π β π§ β πΌππ§β1 ROC: πΌ < π§ < π This example shows that if there is an ROC for an infinite-duration two-sided signal, it is a ring (annular region) in the z-plane. Poles and Zeros The zeros of a π§-transform π are the values of π§ for which π = 0. The poles of a π§-transform are the values of π§ for which π = β.. Zeros - The value(s) for z where P(z)=0. Poles - The value(s) for z where Q(z)=0. Inversion of the π-Transform There are three methods that are often used for the evaluation of the inverse π-transform in practice: Direct evaluation of inverse π-Transform equation, by contour integration. Expansion into a series of terms, in the variables π§, and π§β1 (Power Series Expansion) Partial-fraction expansion and table lookup. The Inverse π-Transform by Partial- Fraction Expansion In the table lookup method, we attempt to express the function π linear combination as a where π1 , β¦ , ππ are expressions with inverse transforms a table π₯1 , β¦ , π₯π available in decomposition is possible, then π₯ , the inverse z-transform of π , can of π§ -transform pairs. If such a easily be found using the linearity property as The Inverse π-Transform by Partial- Fraction Expansion This approach is particularly useful if π π§ is a rational function. Without loss of generality, we assume that π0 = 1, The expression above is called proper if ππ β 0 and π < π. This is equivalent to saying that the number of finite zeros is less than the number of finite poles. The Inverse π-Transform by Partial- Fraction Expansion In general, any improper rational function (π β₯ π) can be expressed as where the degree of π΅1 is less than π΄. The Inverse π-Transform by Partial- Fraction Expansion If we already have our rational expression, Next thing to do is to eliminate negative powers of π§ by multiplying both the numerator and denominator of π§π. This results in, The Inverse π-Transform by Partial- Fraction Expansion To make sure that the transform is proper, we factor out π§ on the numerator to achieve the form, We then express the denominator in factored form to get the partial fraction decomposition of the transform. There are two cases: Distinct poles Repeating poles Distinct Poles Suppose that the poles π1, π2, β¦ , ππ are all different (distinct). Then we seek an expansion of the form, Now the problem is finding the value of the unknown coefficients π΄1, π΄2, β¦ , π΄π. Repeating Poles Suppose that the factored form of the denominator of the rational expression is in the form π, which means that there is π multiplicity of poles. Then we seek an expansion of the form, Inversion of Transform with Real and Distinct Poles For transforms in the form, π = π§ π§ β π1 + π΄2 π΄1 π§ β π2 + β― + π΄π π§ β ππ Where π1, π2, β¦ , ππ are real and distinct. Manipulate into the form, π = π΄1 1 1 β π1 π§β1 + π΄2 1 1 β π2 π§β1 + β― + π΄π 1 1 β ππ π§β1 Inversion of Transform with Real and Distinct Poles Take the inversion on both sides πβ1 = π΄1 π 1 1 β π1π§β1 + π΄2 1 π§ β π2π§β1 + β― + π΄π From the table, πβ1 ππ ππ’ =α ππ’ ππ π ππΆ: π§ > ππ ππ π ππΆ: π§ < ππ Inversion of Transform with Real and Distinct Poles Therefore, π₯ = π΄1ππ + π΄2π2 + β― + π΄πππ π’ 1 2 π If the signal π₯ is causal, the ROC is π§ > ππππ₯ , where ππππ₯ = max. Thus, a causal signal, having a π-transform that contains real and distinct poles, is a linear combination of real exponential signals. Inversion of Transform with Complex Poles For transforms in the form, π = π§ π§ β ππ π΄π β π π§ β πβ Where ππ, πβ are complex. Then its inverse transform is π π₯ = π΄ ππ + π΄β π π’ π π π We have to express π΄π and ππ in complex exponential form π΄π = π΄π πππΌπ ππ = πππππ½π Where πΌπ and π½π are phases of π΄π and ππ. Inversion of Transform with Complex Poles Substitute in the inverse transform, π₯ = π΄π π ππ π½ππ+πΌπ + πβπ π½ππ+πΌπ π’ Which is also equal to π₯ Therefore, = 2 π΄π ππ cos π’ πβ1 β π π§ β πβ = 2 π΄π ππ cos π’ if the ROC is π§ > ππ = ππ Inversion of Transform with Double Poles For transforms in the form, Manipulate into the form, π = π§ 2 π΄π π§β1 π = π΄π 2 π΄ π = π ππ πππ§ 2 Inversion of Transform with Double Poles Recall that, πβ1 =α π ππ π ππΆ: π§ βπ Therefore, = π΄π π ππ ππ’ = π΄ππ πβ1π’ ππ < ππ π’ ππ π ππΆ: π§ πβ1 > If the signal π₯ is causal or the ROC is π§ > ππ