logics of the laplace transform
TRANSCRIPT
Page 5-1
LOGICS OF The Laplace Transform BY TARUN GEHLOT
Introduction
(1) System analysis
static system: y(t) = ax(t) => easy (simple processing)
dynamic system:
)(...)()(...)()( )(
01
)1(
1
)(
txbdt
tdxbtyadt
tdyadt
tdymm
m
nn
n
n
n
Can we determine y(t) for given u(t) easily?
Easier solution method
))(()()()()(
1 fYFtyfXfHfY
(1) we have systematic way to obtain H(f) based on the differential equation(2) we can obtain X(f)
Fourier transform: an easier way
(2) ProblemFourier transform of the input signal:
DynamicSystem
x(t) input y(t) output
A processor whichprocesses the input signalto produce the output
DynamicSystem
X(f) Y(f )
H(f )Algebraic equation, notdifferential equation
Page 5-2
1||
)()(
2
2
ftj
ftj
e
dtetxfX
if x(t) does not go to zero when t and t X(f) typically does not exist! (the existence of X(f) if not guaranteed)
A very strong condition, can not be satisfied by many signals!
(3) Solution:
Why should we care about t<0 for system analysis? We do not care!x(t) does not go to zero (when t ), but tetx )( may!
(Will be much easier. ) use “single-sided” Fourier transform of tetx )( , instead of “double-
sided” Fourier transform of x(t).
0 0
)()())(( dtetxdteetx tjtjt
very useful, let’s use a new name for it: Laplace transform.
(4) Laplace Transform
Definition: Laplace transform of x(t)
0
)()()()]([ jsdtetxsXtxL st
What is a Laplace transform of x(t)?A time function? No, t has been eliminated by the integral with respect to t!A function of s ( s is complex variable)
(5) System analysis using Laplace transform
Page 5-3
))(()()()()(
1 sYLtysXsGsY
(6) How is the inverse transform defined?
j
j
stdsesXj
tx
)(
21)(
(7) Will we often use the definition of the inverse transform to find timefunction?
No!What will we do?
Express X(s) as sum of terms for which we know the inverse transforms!
5-2 Examples of Evaluating Laplace Transforms using the definition
(1) x(t)=1 and step function x(t)=u(t)
0(Re(s))1)]([)1(
1)0sin0(cos1)0(,)0(,01|(|
)(1)()]()([
00
00
000
stuLL
sj
s
ifeifee
es
ees
ees
es
e
stdes
dtedtetxtutxL
j
jjt
t
tjtt
t
st
t
t
ststst
(2) )()( tuetx t
0
)(
0
)]([ dtedteetueL tssttt
Define a new complex variable ss~
DynamicSystem
X(s) Y(s )
G(s )
Inverse Laplace transform
Page 5-4
0
~
dte ts
we know 0)Re(1
0
ss
dte st
seL
sorss
tueL
ss
dte
ss
dte
t
t
ts
ts
1][
)Re()Re(0)Re(1)]([
0)Re(1
0)Re(1
0
)(
~
~0
~
(3) )()( ttx
1
)sin(cos
)()]([
0
00
0
tt
ttjt
tst
st
tjte
eee
dtettL
No constraint on s.
5-2B Discussion: Convergence of the Laplace Transform
(1) To assure
00
)()( dteetxdtetx tjtst converge, )Re(s must be psotive
enough such that tetx )( goes to zero when t goes to positive infinite
(2) Region of absolute convergence and pole
Page 5-5
(3) How to obtain Fourier transform form Laplace transform:
))(()()()]([ txFjXsXtxLjs
Important: why introduce Laplace transform; definition of Laplace transform as amodification of Fourier transform; find the Laplace transforms of the three basicfunctions based on the (mathematical) definition of Laplace transform.
Chapter structure
Part one: Definition (5.1)Part two: Direct evaluation of Laplace transforms of simple time-
domain function.Easy? Not at all!
complex (not simple) functions: even harder tools for application of Laplace transform in system analysis
Part three: Rest of the chapter
What tools: tools for easier Laplace transform evaluationtools for easy inverse transform
Page 5-5
(3) How to obtain Fourier transform form Laplace transform:
))(()()()]([ txFjXsXtxLjs
Important: why introduce Laplace transform; definition of Laplace transform as amodification of Fourier transform; find the Laplace transforms of the three basicfunctions based on the (mathematical) definition of Laplace transform.
Chapter structure
Part one: Definition (5.1)Part two: Direct evaluation of Laplace transforms of simple time-
domain function.Easy? Not at all!
complex (not simple) functions: even harder tools for application of Laplace transform in system analysis
Part three: Rest of the chapter
What tools: tools for easier Laplace transform evaluationtools for easy inverse transform
Page 5-5
(3) How to obtain Fourier transform form Laplace transform:
))(()()()]([ txFjXsXtxLjs
Important: why introduce Laplace transform; definition of Laplace transform as amodification of Fourier transform; find the Laplace transforms of the three basicfunctions based on the (mathematical) definition of Laplace transform.
Chapter structure
Part one: Definition (5.1)Part two: Direct evaluation of Laplace transforms of simple time-
domain function.Easy? Not at all!
complex (not simple) functions: even harder tools for application of Laplace transform in system analysis
Part three: Rest of the chapter
What tools: tools for easier Laplace transform evaluationtools for easy inverse transform
Page 5-6
5-3 Some Laplace Transform theorems(Tools for evaluating Laplace transform based on the Laplace
transforms of the basic functions)
5.3.1 LinearityAssume )()()( 2211 txatxatx ( 1a and 2a are time independent)
)]([)()],([)( 2211 txLsXtxLsX then )()()]([)( 2211 sXasXatxLsX
HW#2-1: Assume )()()()()( 2211 txtatxtatx , )]([)( 11 txLsX and )]([)( 22 txLsX .
(a) Is )]([)( txLsX equal to )()()()( 2211 sXtasXta ?(Answer: Yes or No)
(b) If )]([)( 11 taLsA , is it true)()()()()]([ 2211 sXsAsXsAtxL ?
(Answer: Yes or No)
Example 5.1(1) Find )(cos 0tL
Key to solution : express )(cos 0t as linear combination of )(t , )(tu ,and/or te :
seL
stuL
tL
t 1][
1)]([
1)]([
let 0 j
0
1][ 0
jseL tj
let 0 j
0
)( 1][][ 00
jseLeL tjtj
Page 5-7
Can we use tje 0 and tje 0 to express )cos( 0t ?
)sin()cos(
)sin()cos()sin()cos(
00
00
00
0
0
tjte
tjttjte
tj
tj
20
2
00
00
00
0
0
0
))(()()(
21
1121
)]()([21)][cos(
2)cos(
)cos(2
00
00
00
ss
jsjsjsjs
jsjs
eLeLtL
eet
tee
tjtj
tjtj
tjtj
(2) Find ][sin 0tL
5-3-2 Transforms of Derivatives
Assume )]([)( txLsX
Then )0()()(
xssX
dttdxL
Proof:
(1) Definition
00
)()()()( tdxedte
dttdx
tdtdxL stst
(2) Integration by parts:General equation:
Page 5-8
b
a
bt
at
b
a
tdutvtvtutdvtu )()()()()()(
(3) Use the above equation
Why? If we assumestetutxtv )(,)()(
dtetxsdetxtdutv stst
000
)()()()(
)()( txLsX
](1)from)([)()()(
)()(,)(
00
dttdxLtdxetdvtu
txtvetu
st
st
)]([)(
)()(
)()()()(
0
00
0
txsLtxe
dtetxstxe
tdutvtvtu
t
tst
stt
tst
b
a
t
t
)(lim txe st
t
must go to zero. Otherwise,
0
)()]([ dtetxtxL st does not exist !
)0()0()( 00 xxetxe st
tst
use0 as lower limit => )0( x
)0()()()0(
)()()()(0
0
xssXssXx
tdutvtvtu t
t
Page 5-9
HW#2-2: Assume )]([)( txLsX . Prove
)0()0()()( )1(22
xsxsXs
dttxdL
HW#2-3: Express
n
n
dttxdL )()(
using )]([ txL
Example 5-2
Find i(t) using Laplace transform methodfor t>0
Solution:(1) Before switched from 1 to 2 at t=0
AiAi 2)0(224
(2) System equation (t>0)
KVL:0)(2)(
)2()1(0)()(
tidt
tdi
ohmRHLtRidt
tdiL
(3) Solve system equation using Laplace transform
Atuetis
sI
sIssIissI
tiLdt
tdiLtidt
tdiL
t )(2)(2
2)(
02)()2()(2)0()(
)]([2)()(2)(
2
Page 5-10
5-3-3 Laplace Transform of an integral
Assume )]([)(,)()( txLsXdxtyt
Thens
yssXdxL
t )0()()(
where
0
)()0( dxy
Proof :
00
0
0
0
)()(
vduuvudv
dtedxdxL
tt
stt
(1)
sy
dxs
edxse
sedxuv
stst
t
t
t
sttt
t
)0(
)()(lim
)(
00
00
(2)
)(1)(1)(000
sXs
dtetxs
dttxs
evdu stst
(3)
sy
ssX
ssX
sydxL
t )0()()()0()(
Proved!
0
1
)0( y
Page 5-11
Example 5.3:
Find I(s) = L(i(t))
Solution:(1) Differential equationKVL :
)()()()( tvtvtvtx RCL
t
CC
t
CC
tt
C
C
C
diC
tvv
diC
vtv
diC
dv
dttiC
tdv
dttdvCti
)(1)(0)(
)(1)()(
)(1)(
)(1)(
)()(
)()(
)(1)(
)()(
tRitv
diC
tv
dttdiLtv
R
t
C
L
(2) Laplace transform
)()(
)0(1)(1
)(11)(1
)(1)(1)(
)0()()]0()([)(
)()()()(
0
0
sRIsV
vs
sICs
dics
sICs
diss
sIC
sV
zeroisLsIissILsV
sVsVsVsX
R
c
C
L
RCL
Page 5-12
LCs
LRsL
vssX
sRC
Ls
vssX
RCs
Ls
vs
sXsI
sRIvs
sICs
sLsIsX
C
C
C
C
1)0()(
1)0()(
1
)0(1)()(
)()0(1)(1)()(
2
2
5-3-4. Complex Frequency shift (s-shift) Theorem
Assume tetxty )()()]([)()]([)( tyLsYtxLsX
Then )()( sXsY
setuL
stuL t 1])([,1)]([
20
20
020
20 ][sin][cos
s
tLs
stL
=>2
020
020
20 )(][sin
)(][cos
×
×
setL
ssetL tt
Example 5-4 Find136
8)]([)( 211
sssLsXLtx
Solution:
2222
22
2)3(2)2/5(
2)3(3
4965)3(
1368)(
´
sss
sss
ssssX
Page 5-13
)0(2sin252cos)]([)( 331 ttetesXLtx tt
5-3-4 Delay Theorem question: How to express delayed function?
Assume )()]()([)]([ sXtutxLtxL
Then )0()()]()([ 0000 tsXettuttxL st
(If )0( 0 t , it will not be a delay!)Proof :
)()()(
)()(
)()(
)()()()(
)()(
)]()([
0000
0
00
0
00
0
0
0
00
0)(
0
)(00
000
00
000
00
sXedtetxedexe
ttdettxe
dtettxdtettx
dtettuttxdtettuttx
dtettuttx
ttuttxL
stststssttt
t
ttsst
t
sttts
t
st
t
stt
st
st
Page 5-14
Question: will )()]()([ 000 sXettuttxL st be true if ?00 t
No! (it will not be a delay)
Example 5-5: Square wave beginning at t = 0
sT
sT
e
sTsTsTsT
sq
e
essss
ss
sssss
es
es
es
ess
txL
sT
2
2
32
432
223
2
0
0
021
00
00
1
11111
)1(21
...)(21
...121212121
121212121)]([
5-3-5 ConvolutionSignal 1: )(1 tx Signal 2 : )(2 tx
dtxxtxtxty
)()()(*)()( 2121
if 00)(1 ttx
dtxxty
0
21 )()()(
Page 5-15
if )0)((00)( 22 ttxttx
dtxxtyt
0
21 )()()(
Therefore, if 00)(,0)( 21 ttxtx
dtxxdtxxdtxxt
)()()()()()( 210
210
21
])()([])()([])()([ 210
210
21 dtxxLdtxxLdtxxLt
0 0
210 0
21 ])()[(])()([ ddtetxxdtedtxx stst
Look at
)()(
)(
)()(
20
2
00)(
2
0
)(2
02
2
0
sXedexe
dexe
dteetxdtetx
sssx
ss
dtd
t
stsst
tt
Then
)()(
)()(
)()()(
21
012
021
sXsX
dexsX
dsXexsY
s
s
t
Page 5-16
5-3-7 Product5-3-8 Initial Value Theorem
)(lim)0(
)]([)( 1
ssXx
sXLtx
s
Example: A demonstration where x(0) is obvious)(cos)( 0 ttuetx t
It is evident: 10cos)0( 00 ex
Using Laplace transform
20
2)()]([)(
sstxLsX
122lim
/)22(/)2(lim
222lim
/)2(/)(lim
2lim
)()(lim)(lim)0(
20
22
2
20
22
2
20
2
sss
s
s
ss
dssddssd
ss
dsssddsssd
ssss
sssssXx
5-3-9 Final Value Theorem: if )(tx and dttdx /)( are Laplace transformable, then)(lim)(lim
0ssXtx
st
(condition: )(ssX has no poles on axisj or in the right-half s-planor )(lim txt exists)
5-3-10 Scalinga>0: x(at) a times fast (if a>1)
or slow (if a<1) as x(t)
)]([)( txLsX
What do we expect on )]([ atxL ?
Page 5-17
?)()]([asXatxL
asX
adex
a
atdeatxa
dteatxatxL
as
ta
at
atasa
st
1)(1
)()(1)()]([
00
0
)(0
0
5-4 Inversion of Rational Functions(1) Ways to find )(tx from )(sX
(1)
dtesX
jtx st)(
21)( (Contour Integral)
(2) Transform pair
)(1
)(1
tues
tus
t
Therefore )()(1)( tuetxs
sX t
(2) All kinds of Laplace Transform ? No!
We almost only see
s
nnnn
mmmm
easasas
bsbsbsb
11
1
11
10
...
...
rational function X(s) Delay
)()(])([)(
)]([)(1
1
tutxesXLty
sXLtxs
Page 5-18
Consider Rational Functions only!
(3) Non proper Rational Functionproper Rational Function
Non proper m>=n )0( 0 bproper m<n
Non proper => proper + Polynomial (using long division)
2351
23764
22
23
ss
ssss
sss
53
74764
1
2
2
23 232
ssss
sssss
sss
How to find inverse Laplace transform for polynomials?
)()()1()()1()(
)1(111
)(
ttLsLsLts nn
consider proper rational functions only!
(4) Proper Rational Functions: Partial Fraction Expansion
sum of
t
t
t
tn
n
es
tus
t
ttues
ttues
s
tunet
s
1
)(1)(1
)(sin)(
)(cos)(
)(!)(
1
020
20
020
2
1
Page 5-19
Let’s look at examples, and then summarize!
Techniques:Common Denominator Factorize first!Specific value of s Expand second!Heaviside’s Expansion Find coefficients third!Matlab
Example 5-9: Simple Factors
161010)( 2
ss
sY
Solution:
(1) Factorize and expand28)2)(8(
10)(
s
Bs
Ass
sY
(2) Common Denominator Methods
3/53/56/1010821082
010)8()2(
)2)(8()8()2(
)2)(8(10
ABBBBA
BABAsBsA
sssBsA
ss
)()35
35()(
21
35
81
35)(
28 tueety
sssY
tt
specific values of s
41041010
282810
28)2)(8(10
2
0
BA
BAs
Bs
Ass
s
s
Can you solve for A and B?
Page 5-20
Heaviside Expansion
3/528
102
)8(2
1028)2)(8(
10
8
AssBA
s
sB
sA
sss
and 3/582
108
)2(8
10 2
BBssA
s
s
Example 5-10 Imaginary Roots
)8)(2)(1(202515)( 2
2
sss
sssY
Solution: what do we have:
82)( 4321
sA
sA
jsA
jsAsY
821)()(
821)()(
)(
432
1221
432
21
sA
sA
sjAAsAA
sA
sA
sjsAjsAsY
A1+A2 must be real number(-A1+A2)j must be real number
821)( 43
221
sA
sA
scscsY
Heaviside Expansion => A3=1 and A4= - 2.
82
21
1)8)(2)(1(202515)( 2
212
2
ssscsc
ssssssY
s=1 =>92
31
2932202515 21
´́ cc
s=2 => 102
41
52
104520225415 21
cc
Same as real roots!
Page 5-21
Can we solve for c1 and c2?c1=1 c2=1
82
21
11
1
82
21
11)(
22
2
sssss
sssssY
=> )(]2sin[cos 82 tueett tt Too complex: use MATLAB
Example 5-11 Repeated linear Factors
2321
2
)2(28
)8()2(10)(
sA
sA
sA
ssssY
Example 5-12
34
2321
3
)2()2(28
)8()2(10)(
sA
sA
sA
sA
ssssY
Example 5-13 Complex - Conjugate Factors
jsA
jsA
sA
ssss
ssssssY
112]1)1)[(2(662
)22)(2(662)(
3212
2
2
2
Example 5-14 Repeated Quadratic Factors
Page 5-22
2222
2111
22
234
)1(12
)1)(2(157125)(
scsB
scsB
sA
sssssssY
* Summary of Partial–Fraction Expansion(1) Expansion Structure:
Simple Roots (including complex conjugate)
=>j
j
sA
could be complex.
Repeated Roots: m multiplicity
=> mj
m
jj sB
sB
sB
)(...
)( 221
real number or complex number
(2) Avoid complex numberFor complex conjugates: jbaj
kkj
kk
j
k
j
j
j
j
basDcs
s
Bs
B
basDcs
sA
sA
])[()(
)(
22*
*
22*
*
(3) Inverse Laplace transform
2)()!1()(
)(
1
ktuk
etAs
A
tueAs
A
tk
kkj
j
tj
j
j
j
j
Page 5-23
)(]sin(cos)sin(cos[)!1(
)(][)!1()()(
1
1
*
*
*
tubtjbtBbtjbtAekt
tueBeAkt
sB
sA
jjat
kjba
jba
tj
tj
k
kj
jk
j
j
j
j
jj
Page 5-24
Page 5-25
Page 5-26