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Page 1: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Signals and Systems

EE235

Page 2: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Today’s menu

• Laplace Transform

Page 3: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Laplace properties (unilateral)

Linearity: f(t) + g(t) F(s) + G(s)

Time-shifting:

FrequencyShifting:

Differentiation:

and

Time-scaling

a

sFa

1

Page 4: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Laplace properties (unilateral)

Multiplication in time Convolution in Laplace

Convolution in time Multiplication in Laplace

Initial value theorem

Final value theorem Final value result

Only works ifAll poles of sF(s) in LHP

Page 5: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Laplace transform table

Page 6: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Another Inverse Example

• Example, find h(t) (assuming causal):

• Using linearity and partial fraction:

Page 7: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Another Inverse Example

• Here is the reason:

Page 8: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Another Inverse Example

• Example, find z(t) (assuming causal):

• Same degrees order for P(s) and Q(s)

• From table:

Page 9: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Inverse Example (Partial Fraction)

• Example, find x(t):

• Partial Fraction

• From table:

Page 10: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Inverse Example (almost identical!)

• Example, find x(t):

• Partial Fraction (still the same!)

• From table:

Page 11: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Output

• Example:

• We know:

• From table (with ROC):

Page 12: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

All tied together

• LTI and Laplace

• So:

LTI

LTIx(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)

Page 13: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Laplace & LTI Systems

• If:

• Then

LTI

LTI

Laplace of the zero-state (zero initialconditions) response

Laplace of the input

Page 14: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Laplace & Differential Equations

• Given:

• In Laplace:– where

• So:

• Characteristic Eq:– The roots are the poles in s-domain, the “power” in time domain.

012

2

012

2

)(

)(

bsbsbsP

asasasQ

0)( sQ

Page 15: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Laplace & Differential Equations

• Example (causal LTIC):

• Cross Multiply and inverse Laplace:

Page 16: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Laplace Stability Conditions

• 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 jw-axis• LTIC system is if marginally stable : poles in the LHP +

unrepeated poles on the j -w axis.

Page 17: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Laplace Stability Conditions

• Generally: system H(s) stability conditions:• The system’s ROC includes the j -w axis• Stable? Causal?

σ

x

x

x

Stable+Causal Unstable+Causal

σ

x

xx

x

x

x

Stable+Noncausal

Page 18: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Laplace: Poles and Zeroes

• Given:

• Roots are poles:

• Roots are zeroes:

• Only poles affect stability

• Example:

Page 19: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Laplace Stability Example:

• Is this stable?

Page 20: Leo Lam © 2010-2013 Signals and Systems EE235. Today’s menu Leo Lam © 2010-2013 Laplace Transform

Leo Lam © 2010-2013

Laplace Stability Example:

• Is this stable?