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Montek Singh Thurs., Feb. 19, :30-4:45 pm, SN115

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Presentation on theme: "Montek Singh Thurs., Feb. 19, :30-4:45 pm, SN115"— Presentation transcript:

1 Montek Singh Thurs., Feb. 19, 2002 3:30-4:45 pm, SN115
The Laplace Transform Montek Singh Thurs., Feb. 19, :30-4:45 pm, SN115

2 What we will learn The notion of a complex frequency
Representing a signal in the frequency domain Manipulating signals in the frequency domain

3 Complex Exponential Functions
Complex exponential = est, where s =  + j Examples: <0, =0 >0, =0 =0, =0 Re(est) =0 <0 >0

4 Some Useful Equalities

5 The Laplace Transform: Overview
Key Idea: Represent signals as sum of complex exponentials since all exponentials have the form Aest, it suffices to know the value of A for each s, to completely represent the original signal i.e., representation transformed from “t” to “s” domain Benefits: Complex operations in the time domain get transformed into simpler operations in the s-domain e.g., convolution, differentiation and integration in time  algebraic operations in the s-domain! Even fairly complex differential equations can be transformed into algebraic equations

6 The Laplace Transform F(s) = Laplace Transform of f(t):
1-to-1 correspondence between a signal and its Laplace Transform Frequently, only need to consider time t > 0:

7 Example 1: The Unit Impulse Function
F(s) = 1 everywhere!

8 Example 2: The Unit Step Function

9 Some Useful Transform Pairs

10 Properties of the Laplace Transform (1)

11 Properties of the Laplace Transform (2)


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