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Signals and Systems Chapter 4 the Laplace Transform.

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Presentation on theme: "Signals and Systems Chapter 4 the Laplace Transform."— Presentation transcript:

1

2 Signals and Systems

3 Chapter 4 the Laplace Transform

4 4.4 The Inverse Laplace Transform

5 Review Multiplying both sides by s =σ+ jω , ds =jdω The Inverse Laplace Transform:

6  This equation states that x(t) can be represented as a weighted integral of complex exponentials.  The contour of integration is the straight line in the s-plane corresponding to all points s satisfying Re(s)=  The formal evaluation of the integral for a general X(s) requires the use of contour integration ( 围线积分 ) in the complex plane,a topic that we will not consider here.  The inverse Laplace transform can be determined by partial-fraction expansion.

7 For example:determine x(t). Firstly, perform a partial-fraction expansion to obtain: Secondly, evaluate the coefficients: thus,the partial-fraction expansion for X(s) is : So,

8 Partial-fraction Expansion  The procedure consists of expanding the rational algebraic expression into a linear combination of lower order terms.

9 Assuming no multiple-order poles and that the order of the denominator polynomial is greater than the order of the numerator polynomial,we can expand X(s) in the form: ROC σ> -a i (right sided signal) σ< -a i (left sided signal) Adding the inverse transforms of the individual terms,then yields the inverse transform of X(s).

10 Discussing 1 : no multiple-order poles,the first order different poles,real numbers or complex numbers

11 For example:

12

13 Homework  Page 250 #4-4(3)(6)(9)(15)


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