2012/12/24 1 Applications of Laplace Transforms • Introduction • Circuit Element Models • Circuit Analysis • Transfer Functions • State Variables • Network Stability • Summary Introduction •To learn how easy it is to work with circuits in the s domain. •To learn the concept of modeling circuits in the s domain. •To learn the concept of transfer function in the s domain. •To learn how to apply the state variable method for analyzing linear systems with multiple inputs and multiple outputs. •To learn how the Laplace transform can be used in stability analysis.
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Applications of Laplace Transforms...2012/12/24 2 Circuit Element Models •Steps in applying the Laplace transform: –Transform the circuit from the time domain to the s domain (a
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2012/12/24
1
Applications of LaplaceTransforms
•Introduction•Circuit Element Models•Circuit Analysis•Transfer Functions•State Variables•Network Stability•Summary
Introduction•To learn how easy it is to work with circuits in the s
domain.•To learn the concept of modeling circuits in the s
domain.•To learn the concept of transfer function in the s
domain.•To learn how to apply the state variable method for
analyzing linear systems with multiple inputs andmultiple outputs.•To learn how the Laplace transform can be used in
stability analysis.
2012/12/24
2
Circuit Element Models•Steps in applying the Laplace transform:
–Transform the circuit from the time domain to the sdomain (a new step to be discussed later).
–Solve the circuit using circuit analysis technique(nodal/mesh analysis, source transformation, etc.).
–Take the inverse Laplace transform of the solutionand thus obtain the solution in the time domain.
s-Domain Models for R and L
)()()()(
)()(resistor,aFor
sRIsVtRiLtvL
tRitv
(b))0(
)(1
)(or
(a))0()(
)0()()(
.)(
)(inductor,anFor
si
sVsL
sI
LissLI
issILsVdt
tdiLtv
Time domain (a) (b)
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3
s-Domain Model for C
(b))0(
)(1
)(or
(a))0()(
)0()()(
.)(
)(capacitor,aFor
sv
sIsC
sV
CvssCV
vssVCsIdt
tdvCti
Time domain (a) (b)
For inductor: For capacitor:
si
sVsL
sI)0(
)(1
)(
)0()()( LissLIsVs
vsI
sCsV
)0()(
1)(
)0()()( CvssCVsI
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Summary
Element Z(s)
Resistor R
Inductor sL
Capacitor 1/sC
*Assuming zero initial conditions
•Impedance in the s domain.–Z(s)=V(s)/I(s)
•Admittance in the s domain.–Y(s)=1/Z(s)=I(s)/V(s)
Example 1
)(2sin2
3)(
)2()4(2
23
1883
)(
1883
4
22
22
232
tutetv
s
sssIsV
sssI
to
o
03
53
033
11
:analysismeshApplying(2)
31)F
31
(
)H1(
1)(
:domainthetion toTransforma(1)
21
21
Is
sIs
Is
Iss
ssCZ
ssLZs
tu
s
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Example 2
V5)0( ov
)0(oCv
Example 2 (Cont’d)
)()1510()(
15)()2(
10)()1(
method,residuetheApplying
2
2
1
||
tueetv
sVsB
sVsA
tto
so
so
21)2)(1(3525
10105.02
10)1(10
:nodeatanalysisnodalApplying
sB
sA
sss
V
sVVVsa
o
ooo
a
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6
0)0( Ii
Example 3
)()()0(
,)(
)()()(
0))((
/
0/00
000
0000
00
ieii
RL
RV
eRV
Iti
LRsRVI
sRV
LRssLVsI
sLRsV
sLRLI
sI
sV
LIsLRsI
t
t
Circuit Analysis•Operators (derivatives and integrals) into
simple multipliers of s and 1/s.
•Use algebra to solve the circuit equations.
•All of the circuit theorems and relationshipsdeveloped for dc circuits are perfectly valid inthe s domain.
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Example 1
V5)0(A1)0(
10
C
L
s
vi
sV
)(10 tu
)(3035)(
230
135
)2)(1(540
0)1.0(1
)0()0(5
0310
haveweanalysisnodalusingBy
21
1
111
tueetv
sssss
V
ssvV
si
sVVV
tt
s
Example 2
)(3035
)()101030()51030(
)()()()(
)(105)(
210
15
)2)(1(5
)(1010)(
210
110
)2)(1(10
)(3030)(
230
130
)2)(1(30
ion.superpositusingby1exampleSolve
2
2
321
23
3
22
2
21
1
tuee
tuee
tvtvtvtv
tueetv
sssss
V
tueetv
ssssV
tueetv
ssssV
tt
tt
tt
tt
tt
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Example 3Assume that no initial energy is stored.(a) Find Vo(s) using Thevenin’s theorem.(b) Find vo(0+) and vo() by applying the
initial- and final-value theorems.(c) Determine vo(t).
=10u(t)
Example 3: (a)
)4(12550
3255
55
32)32(50
50)32(
502
,32
1002
and
02
05
0)2(10:analysisnodalApplying
use,findTo
50105
11
1
11
ssssV
ZV
ssss
IV
Z
sssV
IIs
V
sV
I
sVIV
s
IVZZss
VV
ThTh
o
sc
ocTh
scx
x
x
scocThTh
Thoc
V1
=0
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9
Example 3: (b), (c)
4125
4125
lim)(lim)(
givestheoremvalue-finalThe
04
125lim)(lim)0(
givestheoremvalue-initialThe)4(
125)(
:(b)Solution
00
sssVv
sssVv
sssV
soso
soso
o
)()1(25.31)(
25314
125)()4(
25314
125)(
method,residuetheApplying4)4(
125)(
:(c)Solution
4
4
0
tuetv
.sVsB
.ssVA
sB
sA
sssV
to
so
so
o
|
|
Transfer Functions•The transfer function H(s) is the ratio of the output
response Y(s) to the input excitation X(s), assumingall initial conditions are zero.
Example 3Find(a) H(s) = Vo/Vi,(b) the impulse response,(c) the response when vi(t) = u(t) V,(d) the response when vi(t) = 8cos2t V.
Example 3: (a), (b)
i
i
iab
abo
Vss
Vss
ss
Vs
sV
Vs
V
321
)2()1(1)2()1(
)1(||11)1(||1
11
division,By voltage:Solution
)(5.0)(
231
21
321
)(
32321
11
23 tueth
ssVV
sH
sV
Vss
sV
t
i
o
iio
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13
Example 3: (c), (d)
V)(131
)(
31
,31
23
23
2
1
)()()(
1)()()(
(c):Sol
23 tuetv
BA
s
BsA
ss
sVsHsVs
sVtutv
to
io
ii
V)(2sin34
2cos2524
)(
42
34
4231
2524
)(
2564
,2524
,2524
423
423
4
)()()(4
8)(2cos8)(
(d):Sol
23
22
22
2
tuttetv
sss
ssV
CBA
sCBs
s
A
ss
s
sVsHsVs
ssVttv
to
o
io
ii
State Variables•The state variables are those variables which, if
known, allow all other system parameters to bedetermined by using only algebraic equations.
•In an electric circuit, the state variables are theinductor current and the capacitor voltage sincethey collectively describe the energy state of thesystem.