eleg 3124 systems and signals ch. 3 laplace transform · 3 introduction • why laplace transform?...
TRANSCRIPT
![Page 1: ELEG 3124 SYSTEMS AND SIGNALS Ch. 3 Laplace Transform · 3 INTRODUCTION • Why Laplace transform? – Frequency domain analysis with Fourier transform is extremely useful for the](https://reader033.vdocuments.us/reader033/viewer/2022052808/6073510a82ffca2a24207498/html5/thumbnails/1.jpg)
Department of Electrical EngineeringUniversity of Arkansas
ELEG 3124 SYSTEMS AND SIGNALS
Ch. 3 Laplace Transform
Dr. Jingxian Wu
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OUTLINE
• Introduction
• Laplace Transform
• Properties of Laplace Transform
• Inverse Lapalace Transform
• Applications of Laplace Transform
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INTRODUCTION
• Why Laplace transform?
– Frequency domain analysis with Fourier transform is extremely
useful for the studies of signals and LTI system.
• Convolution in time domain Multiplication in frequency
domain.
– Problem: many signals do not have Fourier transform
0),()exp()( atuattx )()( ttutx
– Laplace transform can solve this problem
• It exists for most common signals.
• Follow similar property to Fourier transform
• It doesn’t have any physical meaning; just a mathematical tool
to facilitate analysis.
– Fourier transform gives us the frequency domain
representation of signal.
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OUTLINE
• Introduction
• Laplace Transform
• Properties of Laplace Transform
• Inverse Lapalace Transform
• Applications of Fourier Transform
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LAPLACE TRANSFORM: BILATERAL LAPLACE TRANSFORM
• Bilateral Laplace transform (two-sided Laplace transform)
,)exp()()(
dtsttxsX B
– is a complex variable
– s is often called the complex frequency
– Notations:
– : a function of time t x(t) is called the time domain signal
– a function of s is called the s-domain signal
– S-domain is also called as the complex frequency domain
js
)()( sXtx B
js
)]([)( txLsXB
)(tx
:)(sX B)(sX B
• Time domain v.s. S-domain
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LAPLACE TRANSFORM
• Time domain v.s. s-domain
– : a function of time t x(t) is called the time domain signal
– a function of s is called the s-domain signal
• S-domain is also called the complex frequency domain
– By converting the time domain signal into the s-domain, we can
usually greatly simplify the analysis of the LTI system.
– S-domain system analysis:
• 1. Convert the time domain signals to the s-domain with the
Laplace transform
• 2. Perform system analysis in the s-domain
• 3. Convert the s-domain results back to the time-domain
6
)(tx
:)(sX B)(sX B
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• Example
– Find the Bilateral Laplace transform of )()exp()( tuattx
• Region of Convergence (ROC)
– The range of s that the Laplace transform of a signal converges.
– The Laplace transform always contains two components
• The mathematical expression of Laplace transform
• ROC.
LAPLACE TRANSFORM: BILATERAL LAPLACE TRANSFORM
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• Example
– Find the Laplace transform of )()exp()( tuattx
,1
)(as
sX B
as )Re( ,1
)(as
sX B
as )Re(
LAPLACE TRANSFORM: BILATERAL LAPLACE TRANSFORM
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• Example
– Find the Laplace transform of )()exp(4)()2exp(3)( tuttuttx
LAPLACE TRANSFORM: BILATERAL LAPLACE TRANSFORM
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LAPLACE TRANSFORM: UNILATERAL LAPLACE TRANSFORM
• Unilateral Laplace transform (one-sided Laplace transform)
0)exp()()( dtsttxsX
– :The value of x(t) at t = 0 is considered.
– Useful when we dealing with causal signals or causal systems.
• Causal signal: x(t) = 0, t < 0.
• Causal system: h(t) = 0, t < 0.
– We are going to simply call unilateral Laplace transform as
Laplace transform.
0
0)exp()()( dtsttxsX
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• Example: find the unilateral Laplace transform of the
following signals.
– 1. Atx )(
– 2. )()( ttx
LAPLACE TRANSFORM: UNILATERAL LAPLACE TRANSFORM
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• Example
– 3. )2exp()( tjtx
– 4.
)2sin()( ttx – 5.
)2cos()( ttx
LAPLACE TRANSFORM: UNILATERAL LAPLACE TRANSFORM
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Department of Engineering Science
Sonoma State University
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LAPLACE TRANSFORM: UNILATERAL LAPLACE TRANSFORM
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OUTLINE
• Introduction
• Laplace Transform
• Properties of Laplace Transform
• Inverse Lapalace Transform
• Applications of Fourier Transform
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PROPERTIES: LINEARITY
• Linearity
– If
– Then
The ROC is the intersection between the two original signals
)()( 11 sXtx )()( 22 sXtx
)()()()( 2121 sbXsaXtbxtax
• Example
– Find the Laplace transfrom of )()exp( tubtBA
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PROPERTIES: TIME SHIFTING
• Time shifting
– If and
– Then
The ROC remain unchanged
)()( sXtx
)exp()()()( 000 stsXttuttx
00 t
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PROPERTIES: SHIFTING IN THE s DOMAIN
• Shifting in the s domain
– If
– Then )()exp()()( 00 ssXtstxty
• Example
– Find the Laplace transform of )()cos()exp()( 0 tutatAtx
)Re(s)()( sXtx
)Re()Re( 0ss
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PROPERTIES: TIME SCALING
• Time scaling
– If
– Then
)()( sXtx
1}Re{ as
a
sX
aatx
1)(
1}Re{ s
• Example
– Find the Laplace transform of )()( atutx
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PROPERTIES: DIFFERENTIATION IN TIME DOMAIN
• Differentiation in time domain
– If
– Then
)()( sGtg
)0()()( gssG
dt
tdg
• Example
– Find the Laplace transform of ),(sin)( 2 tuttg
)0()0()0()()( )1()2(1 nnnn
n
n
gsggssGsdt
tgd
0)0( g
)0(')0()()( 2
2
2 gsgsGs
dt
tgd
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PROPERTIES: DIFFERENTIATION IN TIME DOMAIN
• Example
– Use Laplace transform to solve the differential equation
,0)(2)('3)('' tytyty 3)0( y 1)0(' y
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PROPERTIES: DIFFERENTIATION IN S DOMAIN
• Differentiation in s domain
– If
– Then
)()( sXtx
n
nn
ds
sXdtxt
)()()(
• Example
– Find the Laplace transform of )(tut n
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PROPERTIES: CONVOLUTION
• Convolution
– If
– Then
The ROC of is the intersection of the ROCs of X(s)
and H(s)
)()( sXtx )()( sHth
)()()()( sHsXthtx
)()( sHsX
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PROPERTIES: INTEGRATION IN TIME DOMAIN
• Integration in time domain
– If
– Then
)()( sXtx
)(1
)(0
sXs
dxt
• Example
– Find the Laplace transform of )()( ttutr
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PROPERTIES: CONVOLUTION
• Example
– Find the convolution
a
atrect
a
atrect
22
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PROPERTIES: CONVOLUTION
• Example
– For a LTI system, the input is , and the
output of the system is
)()2exp()( tuttx
)()3exp()2exp()exp()( tutttty
Find the impulse response of the system
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PROPERTIES: CONVOLUTION
• Example
– Find the Laplace transform of the impulse response of the LTI
system described by the following differential equation
)()('3)()('3)(''2 txtxtytyty
assume the system was initially relaxed ( )0)0()0( )()( nn xy
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PROPERTIES: MODULATION
• Modulation
– If
– Then
)()( sXtx )()( sXtx
)()(2
1)cos()( 000 jsXjsXttx
)()(2
)sin()( 000 jsXjsXj
ttx
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PROPERTIES: MODULATION
• Example
– Find the Laplace transform of )()sin()exp()( 0 tutattx
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PROPERTIES: INITIAL VALUE THEOREM
• Initial value theorem
– If the signal is infinitely differentiable on an interval around
then
)(tx )0( x
)(lim)0( ssXxs
– The behavior of x(t) for small t is determined by the behavior of X(s) for large s.
s must be in ROC
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PROPERTIES: INITIAL VALUE THEOREM
• Example
– The Laplace transform of x(t) is
Find the value of ))((
)(bsas
dcssX
)0( x
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PROPERTIES: FINAL VALUE THEOREM
• Final value theorem
– If
– Then:
)()( sXtx
)(lim)(lim0
ssXtxst
• Example
– The input is applied to a system with transfer
function , find the value of
0s must be in ROC
)()( tAutx
cbss
csH
)()(
)(lim tyt
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PROPERTIES
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OUTLINE
• Introduction
• Laplace Transform
• Properties of Laplace Transform
• Inverse Lapalace Transform
• Applications of Fourier Transform
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INVERSE LAPLACE TRANSFORM
• Inverse Laplace transform
01
1
1
01
1
1)(asasasa
bsbsbsbsX
n
n
n
n
m
mmm
– Evaluation of the above integral requires the use of contour
integration in the complex plan difficult.
• Inverse Laplace transform: special case
– In many cases, the Laplace transform can be expressed as a
rational function of s
– Procedure of Inverse Laplace Transform
• 1. Partial fraction expansion of X(s)
• 2. Find the inverse Laplace transform through Laplace
transform table.
j
jdsstsX
jtx
)exp()(
2
1)(
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INVERSE LAPLACE TRANSFORM
• Review: Partial Fraction Expansion with non-repeated
linear factors
321
)(as
C
as
B
as
AsX
1
)()( 1 assXasA
2
)()( 2 assXasB
3
)()( 3 assXasC
• Example
– Find the inverse Laplace transform of sss
ssX
43
12)(
23
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INVERSE LAPLACE TRANSFORM
• Example
– Find the Inverse Laplace transform of 23
2)(
2
2
ss
ssX
• If the numerator polynomial has order higher than or equal to the order
of denominator polynomial, we need to rearrange it such that the
denominator polynomial has a higher order.
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INVERSE LAPLACE TRANSFORM
• Partial Fraction Expansion with repeated linear factors
bs
B
as
A
as
A
bsassX
1
2
2
2 )()(
1)(
as
sXasA
)(2
2 as
sXasds
dA
)(2
1
bssXbsB
)(
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INVERSE LAPLACE TRANSFORM
• High-order repeated linear factors
bs
B
as
A
as
A
as
A
bsassX
N
N
N
)()()()(
1)(
2
21
bs
sXbsB
)(
as
N
kN
kN
k sXasds
d
kNA
)()!(
1Nk ,,1
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OUTLINE
• Introduction
• Laplace Transform
• Properties of Laplace Transform
• Inverse Lapalace Transform
• Applications of Laplace Transform
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APPLICATION: LTI SYSTEM REPRESENTATION
• LTI system
– System equation: a differential equation describes the input output
relationship of the system.
)()()()()()()( 0
)1(
1
)(
0
)1(
1
)1(
1
)( txbtxbtxbtyatyatyaty M
M
N
N
N
M
m
m
m
N
n
n
n
N txbtyaty0
)(1
0
)()( )()()(
– S-domain representation
)()(0
1
0
sXsbsYsasM
m
m
m
N
n
n
n
N
– Transfer function
1
0
0
)(
)()(
N
n
n
n
N
M
m
m
m
sas
sb
sX
sYsH
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APPLICATION: LTI SYSTEM REPRESENTATION
• Simulation diagram (first canonical form)
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APPLICATION: LTI SYSTEM REPRESENTATION
• Example
– Show the first canonical realization of the system with transfer
function
6116
23)(
23
2
sss
ssSH
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APPLICATION: COMBINATIONS OF SYSTEMS
• Combination of systems
– Cascade of systems
– Parallel systems
)()()( 21 sHsHSH
)()()( 21 sHsHSH
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APPLICATION: LTI SYSTEM REPRESENTATION
• Example
– Represent the system to the cascade of subsystems.
6116
23)(
23
2
sss
ssSH
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APPLICATION: LTI SYSTEM REPRESENTATION
• Example:
– Find the transfer function of the system
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APPLICATION: LTI SYSTEM REPRESENTATION
• Poles and zeros
)())((
)())(()(
11
11
pspsps
zszszssH
NN
MM
– Zeros:
– Poles:
Mzzz ,,, 21
Nppp ,,, 21
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APPLICATION: STABILITY
• Review: BIBO Stable
– Bounded input always leads to bounded output
dtth |)(|
• The positions of poles of H(s) in the s-domain
determine if a system is BIBO stable.
N
N
m ss
A
ss
A
ss
AsH
)()(
2
2
1
1
– Simple poles: the order of the pole is 1, e.g.
– Multiple-order poles: the poles with higher order. E.g.
1s Ns
2s
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48
APPLICATION: STABILITY
• Case 1: simple poles in the left half plane
kk jp 1
0k 22
1
kks
)()sin()exp(1
)( tuttth kk
k
k
))((
1
kkkk jsjs
kk jp 2
dtthk )(
• If all the poles of the system are on the left half plane,
then the system is stable.
![Page 49: ELEG 3124 SYSTEMS AND SIGNALS Ch. 3 Laplace Transform · 3 INTRODUCTION • Why Laplace transform? – Frequency domain analysis with Fourier transform is extremely useful for the](https://reader033.vdocuments.us/reader033/viewer/2022052808/6073510a82ffca2a24207498/html5/thumbnails/49.jpg)
49
APPLICATION: STABILITY
• Case 2: Simple poles on the right half plane
kk jp 1
0k 22
1
kks ))((
1
kkkk jsjs
kk jp 2
)()sin()exp(1
)( tuttth kk
k
k
• If at least one pole of the system is on the right half
plane, then the system is unstable.
![Page 50: ELEG 3124 SYSTEMS AND SIGNALS Ch. 3 Laplace Transform · 3 INTRODUCTION • Why Laplace transform? – Frequency domain analysis with Fourier transform is extremely useful for the](https://reader033.vdocuments.us/reader033/viewer/2022052808/6073510a82ffca2a24207498/html5/thumbnails/50.jpg)
50
APPLICATION: STABILITY
• Case 3: Simple poles on the imaginary axis
)()sin(1
)( tutth k
k
k
0k 22
1
kks ))((
1
kkkk jsjs
• If the pole of the system is on the imaginary axis, it’s
unstable.
![Page 51: ELEG 3124 SYSTEMS AND SIGNALS Ch. 3 Laplace Transform · 3 INTRODUCTION • Why Laplace transform? – Frequency domain analysis with Fourier transform is extremely useful for the](https://reader033.vdocuments.us/reader033/viewer/2022052808/6073510a82ffca2a24207498/html5/thumbnails/51.jpg)
51
APPLICATION: STABILITY
• Case 4: multiple-order poles in the left half plane
)()sin()exp(1
)( tutttth kk
m
k
k
0k stable
• Case 5: multiple-order poles in the right half plane
)()sin()exp(1
)( tutttth kk
m
k
k
0k
0k 0k
unstable
• Case 6: multiple-order poles on the imaginary axis
)()sin(1
)( tuttth k
m
k
k
unstable
![Page 52: ELEG 3124 SYSTEMS AND SIGNALS Ch. 3 Laplace Transform · 3 INTRODUCTION • Why Laplace transform? – Frequency domain analysis with Fourier transform is extremely useful for the](https://reader033.vdocuments.us/reader033/viewer/2022052808/6073510a82ffca2a24207498/html5/thumbnails/52.jpg)
52
APPLICATION: STABILITY
• Example:
– Check the stability of the following system.
136
23)(
2
ss
ssH