5 Laplace Transform
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Transcript of 5 Laplace Transform
THE LAPLACE TRANSFORM
Chapter 5
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Why?
••ThereThere areare DifferentialDifferential EquationsEquations thatthat willwill bebedifficultdifficult forfor usus toto solvesolve justjust knowingknowing whateverwhatevermethodsmethods wewe havehave learntlearnt soso farfar..
••TheThe LaplaceLaplace transformtransform isis usedused toto produceproduce ananeasilyeasily solvablesolvable algebraicalgebraic equationequation fromfrom ananordinaryordinary differentialdifferential equationequation..
••ItIt hashas importantimportant applicationsapplications inin Mathematics,Mathematics,PhysicsPhysics andand EngineeringEngineering..
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Plan
I - Definition and basic properties
II - Inverse Laplace transform and solutions of DE
III - Operational Properties
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I – Definitions and basic properties
At the end of the lesson you should be
able to :
• Define Laplace Transform.
• Find the Laplace Transform of different type of functions using the definition.
Learning objective
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Integral Transform
If f ( t ) is defined for and
is a function of two variables, then the
improper integral
is an integral transform.
0t
dttftsKdttftsKb
b)(),(lim)(),(
00
),( tsK
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If the limit exist, then the integral exists or
is convergent. (In general, the limit will exist
for only certain values of the variable s).
If the limit does not exist, the integral does
not exist and is divergent.
Integral Transform
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Definition: Laplace Transform
Let f be a function defined for
Then the integral
is said to be the Laplace transform of f,
provided that the integral converges.
.0t
dttfetfL st )()(0
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Notations
)()(
;)()(;)()(
sYtyLand
sGtgLsFtfL
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Use the definition to find the values of the following:
}{.2
}1{.1
tL
L
Example 1
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Use the definition to find the values of the following:
}{.3
}{.2
}1{.1
3teL
tL
L
Example 1
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?}1{L
Solution
dteL st 1}1{0
dteL st
0
}1{
Nst
NdteL
0lim}1{
Nst
N s
eL
0
lim}1{
s
eL
sN
N
1lim}1{
sL
1}1{
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?}{tL
Solution
s
evedv
dtdutust
st
dt
22
0
2
110}{
sss
e
s
tetL
stst
dttetL st
0}{
dtess
tetL st
st
00
1}{
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?}{ 3teL Solution
dteeeL tstt 3
0
3 )(
dte tst
0
3
dte ts
0
)3(
0
)3(
)3(s
e ts
0
)3()3(
)3()3(
s
e
s
e tsts
)3(
10
s
)3(
1
s
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Theorem: Transforms of some Basic Functions
22
2222
221
}{sinh.4
}{cosh.7}{sin.3
}{cos.6!
}{.2
1}{.5
1}1{.1
ks
kktL
ks
sktL
ks
kktL
ks
sktL
s
ntL
aseL
sL
n
n
at
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is a Linear TransformL
)}({)}({)}()({ 2121 tgLctfLctgctfcL
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Example2
15)( ttf
Find the Laplace transform of the function
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Example2
}51{ tL
}5{}1{}51{ tLLtL
}{5}1{ tLL
2
15
1
ss
22
551
s
s
ss
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Transform of a Piecewise function
Given
dttfetfL st )()(0
11
101)(
t
ttf
Find
Example 3
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1
1
0
)}({ dtedtetfL stst
1
1
0
11 stst es
es
)0(1
)1(1
ss es
es
Solution
)12(1
ses
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Laplace Transform of a Derivative
Let
0
'' )()( dttfetfL stFind
)()( tfLsF
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Laplace Transform of a Derivative
0
'' )()( dttfetfL st
dttfestfe stst )()(00
)}({)0( tfLsf
)0()( fssF
f(t)v(t)dt fdv
dtsedueu'
stst
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Laplace Transform of a Derivative
dttfetfL st )()(0
dttfestfe stst )()(00
)}({)0(0 ' tfsLf
)]0()([)0( fssFsf
)0()()0( 2 sfsFsf
)0()0()(2 fsfsFs
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Laplace Transform of a Derivative
Theorem
)0(....)0()0()()}({ )1(21)( nnnnn ffsfssFstfL
)()( tfLsF where
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Laplace Transform of a Derivative
Example
tyyy 423 '''
Find the Laplace transform of the following IVP
1000 )( y)y( '
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Laplace Transform of a Derivative
)4()23( ''' tLyyyL
)(4)(2)(3)( ''' tLyLyLyL
Solution tyyy 423 '''
2
'2 4)(2)0()(3)0()0()(
ssYyssYysysYs
2
2 4)(2)(31)(
ssYssYsYs
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2
2 4)(2)(31)(
ssYssYsYs
Laplace Transform of a Derivative
Solution
2
2 41)()23(
ssYss
2
22 4
)()23(s
ssYss
)1(
2
)1)(2(
4)(
22
2
ss
s
sss
ssY
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II – Inverse Laplace Transform and solutions of DEs
At the end of the lesson you should be
able to :
• Define Inverse Laplace Transform.
• Solve ODEs using the Laplace Transform.
Learning objective
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Inverse Transforms
If F (s) represents the Laplace transform of a
function f (t), i.e.,
L {f (t)}=F (s)
then f (t) is the inverse Laplace transform of F (s)
and, )}({)( 1 sFLtf
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Theorem : Some Inverse Transforms
22
1
22
1
22
1
22
1
1
1
11
sinh.4
cosh.7sin.3
cos.6...,3,2,1,!
.2
1.5
11.1
ks
kLkt
ks
sLkt
ks
kLkt
ks
sLktn
s
nLt
asLe
sL
n
n
at
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Application
ts
Ls
L
ts
Ls
Ls
L
6sin6
1
6
6
6
1
36
1.2
60
1!5
!5
212
2.1
22
1
2
1
5
15
1
15
1
6
1
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is a Linear Transform1L
)}({)}({)}()({ 111 sGLsFLsGsFL
Where F and G are the transforms of some functions f and g . This can also extend to any finite combination of Laplace transform
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Division and Linearity
Find
4
432
1
s
sL
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Division and Linearity
22
1
22
1
2
1
2
4
2
3
4
43
sL
s
sL
s
sL
22
1
22
1
2
2)2(
2)3(
sL
s
sL
tt 2sin)2(2cos)3(
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Partial Fractions in Inverse Laplace
Find
)2)(1(
11
ssL
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Partial Fractions in Inverse Laplace
1
1
2
1
)2)(1(
1
ssss
)2)(1(
11
ssL
1
1
2
11
ssL
1
1
2
1 11
sL
sL
tt ee 2
,
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Method to solve DE
DEApply Laplace
transform Lequation in )(sY
Apply Inverse Laplace transform
1L
Solution )(sYSolutionof the initial DE
)(ty
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Example 1
Solve the partial given IVP by
Laplace transform.
3)0(,02 yydt
dy
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Solution 1
3)0(,02 yydt
dy
02
y
dt
dyL
02
yL
dt
dyL
0)()0()(2 sYyssY
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Solution 1
0)()0()(2 sYyssY
06)()12( sYs
12
6)(
ssY
12
6)( 1
sLty
))2
1((2
61
s
L
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Solution 1
)2
1(
13)( 1
s
Lty
23)(t
ety
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Example 2
Solve the given IVP DE by Laplace transform
6)0(,2sin133 ytydt
dy
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Solution 2
tLyLdt
dyL 2sin133
4
213)(3)0()(
2ssYysYs
4
26)(36)(
2
ssYsYs
4
)4(6
4
26)(3
2
2
2
s
s
ssYs
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Solution 2
)4)(3(
506
4
24626
3
1)(
2
2
2
2
ss
s
s
s
ssY
)4)(3(
506)(
2
21
ss
sLty
)4)(3(
)3)(()4(
43)4)(3(
5062
2
22
2
ss
sCBssA
s
CBs
s
A
ss
s
8A 2B 6C……………………
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Solution 2
4
62
3
8
)4)(3(
506)(
2
11
2
21
s
sL
sL
ss
sLty
4
16
42
3
18
2
1
2
11
sL
s
sL
sL
4
2
2
62cos28
2
13
sLte t
tte t 2sin32cos28 3
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III – Operational Properties
At the end of the lesson you should be
able to use translation theorems.
Learning objective
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First translation theorem
)()}({ sFtfL
a
)()}({ asFtfeL at
If
and is any real number, then
.
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First translation theorem
.
}{ 35 teL t
45
45335
)5(
6!3}{}{
ss
tLteLss
sst
Example 1:
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First translation theorem
.
Example 2:
}4cos{ 2 teL t
16)2(
2
4}4{cos}4cos{
22
2222
s
s
s
stLteL
ss
sst
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.
)()}({ asFtfeL at
)}({)}({ 11 asFLtfeLL at
)}({)( 1 asFLtfeat
Inverse form of First translation theorem
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.
Example 1:
2
1
)3(
52
s
sL
22 )3(
11
3
2
)3(
52
sss
s
2
11
2
1
)3(
111
3
12
)3(
52
sL
sL
s
sL
3
2
13
)(
111)1(2
ss
t
sLe
tt tee 33 112
Inverse form of First translation theorem
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Exercise
.0)0(,0)0(,164 yyeyyy t
Solve
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}{}1{}{6}{4}{ teLLyLyLyL
1
11)(6)]0()([4)0()0()(2
sssYyssYysysYs
1
11)(6)(4)(2
sssYssYsYs
Solution
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1
11)()64( 2
sssYss
)1(
12)()64( 2
ss
ssYss
)64)(1(
12)(
2
ssss
ssY
Solution
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)64(1)64)(1(
1222
ss
DCs
s
B
s
A
ssss
s
)64(3
5
21
3
1
6
1
)64)(1(
1222
ss
s
ssssss
s
Solution
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)64(3
5
21
3
1
6
1
)64)(1(
12)(
22
ss
s
ssssss
ssY
})64(
3
5
2{}1
3
1
{}6
1
{)}({2
1111
ss
s
Ls
Ls
LsYL
Solution
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})64(
3
5
2{}1
3
1
{}6
1
{)}({2
1111
ss
s
Ls
Ls
LsYL
}2)2(
2{
23
2}
2)2(
2{
2
1}
1
1{
3
1}
1{
6
1)}({
2
1
2
1111
sL
s
sL
sL
sLsYL
.2sin23
22cos
2
1
3
1
6
1)( 22 teteety ttt
Solution
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Unit Step Function or Heaviside Function
The unit step function is defined as
)( atU
.,1
0,0)(
at
atatU
U
t
1
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When a function, say for ismultiplied by the unit stepfunction “ turn off ” a portion of the graphof that function.
)(tf 0t)( atU
Remark
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What happen when is
multiplied by the Heaviside function
32)( ttf
Example
?)2()( tUtf
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32)( ttf
Example
)2()( tUtf
-3
t
f
t
-3
2
f
0 0
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The Second Translation Theorem
If and then )}({)( tfLsF ,0a
).()}()({ sFeatUatfL as
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Example 1
Let
sLsF
atftf
1}1{)(
1)(1)(
.)}({s
eatUL
as
then
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Example 2
Find
3,2
30,)(
t
t ttg
)3(2))3(1()( tUtUttg
)}({ tgL where
)}.3({2)}3({}{)}({ tULttULtLtgL
)3(2)3( tUttUt
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Example 2
)}.3({2)}3({}{)}({ tULttULtLtgL
.2)}3({1 3
2 s
ettUL
s
s
For We would like to apply the previous theorem )}3({ ttUL
So, we write ttf )3(
3)( ttf
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Example 2
Then
where
)()}3({ 3 sFettUL s
Finally
sstLtfLsF
31}3{)}({)(
2
.1231
)}({3
2
333
2
3
2 s
e
s
e
s
e
s
e
s
e
stgL
sssss
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The Inverse Second Translation Theorem
If then )}({)( 1 sFLtf
).()()}({1 atUatfsFeL as
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Example
Evaluate
}4
1{ 21 se
sL
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