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Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform.

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Presentation on theme: "Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform."— Presentation transcript:

1 Leo Lam © 2010-2013 Signals and Systems EE235

2 Today’s menu Leo Lam © 2010-2013 Laplace Transform

3 Laplace properties (unilateral) Leo Lam © 2010-2013 Linearity: f(t) + g(t) F(s) + G(s) Time-shifting: Frequency Shifting: Differentiation: and Time-scaling

4 Laplace properties (unilateral) Leo Lam © 2010-2013 Multiplication in time Convolution in Laplace Convolution in time Multiplication in Laplace Initial value theorem Final value theorem Final value result Only works if All poles of sF(s) in LHP

5 Laplace transform table Leo Lam © 2010-2013

6 Another Inverse Example Leo Lam © 2010-2013 Example, find h(t) (assuming causal): Using linearity and partial fraction:

7 Another Inverse Example Leo Lam © 2010-2013 Here is the reason:

8 Another Inverse Example Leo Lam © 2010-2013 Example, find z(t) (assuming causal): Same degrees order for P(s) and Q(s) From table:

9 Inverse Example (Partial Fraction) Leo Lam © 2010-2013 Example, find x(t): Partial Fraction From table:

10 Inverse Example (almost identical!) Leo Lam © 2010-2013 Example, find x(t): Partial Fraction (still the same!) From table:

11 Output Leo Lam © 2010-2013 Example: We know: From table (with ROC):

12 All tied together LTI and Laplace So: Leo Lam © 2010-2013 LTI x(t)y(t) = x(t)*h(t) X(s)Y(s)=X(s)H(s) Laplace Multiply Inverse Laplace H(s )= X(s) Y(s)

13 Laplace & LTI Systems Leo Lam © 2010-2013 If: Then LTI Laplace of the zero-state (zero initial conditions) response Laplace of the input

14 Laplace & Differential Equations Leo Lam © 2010-2013 Given: In Laplace: –where So: Characteristic Eq: –The roots are the poles in s-domain, the “power” in time domain.

15 Laplace & Differential Equations Leo Lam © 2010-2013 Example (causal  LTIC): Cross Multiply and inverse Laplace:

16 Laplace Stability Conditions Leo Lam © 2010-2013 LTI – Causal system H(s) stability conditions: LTIC system is stable : all poles are in the LHP LTIC system is unstable : one of its poles is in the RHP LTIC system is unstable : repeated poles on the j-axis LTIC system is if marginally stable : poles in the LHP + unrepeated poles on the jaxis.

17 Laplace Stability Conditions Leo Lam © 2010-2013 Generally: system H(s) stability conditions: The system’s ROC includes the jaxis Stable? Causal? σ jωjω x x x Stable+CausalUnstable+Causal σ jωjω x x x x σ jωjω x x x Stable+Noncausal

18 Laplace: Poles and Zeroes Leo Lam © 2010-2013 Given: Roots are poles: Roots are zeroes: Only poles affect stability Example:

19 Laplace Stability Example: Leo Lam © 2010-2013 Is this stable?

20 Laplace Stability Example: Leo Lam © 2010-2013 Is this stable?


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