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INC341 Root Locus. Lecture 7. Rectangular vs. polar. j ω. s = 4 + j3. 3. σ. 4. Rectangular form:4 + j3 Polar formmagnitude=5, angle = 37. Rectangular form. Add, Subtraction. Polar form. Multiplication. Division. b. r. θ. a. Vector representation of a transfer function. - PowerPoint PPT Presentation
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INC 341 PT & BP
INC341Root Locus
Lecture 7
INC 341 PT & BP
s = 4 + j3
jω
σ
3
4
Rectangular form: 4 + j3
Polar form magnitude=5, angle = 37
Rectangular vs. polar
INC 341 PT & BP
Rectangular form
Add, Subtraction
Polar form
45)1()34( jjj
Multiplication
2510)1237(25
122375
Division
492
5
122375
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jba
a
b
r
θ
r
sin
cos
arctan
22
rb
ra
a
b
bar
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Vector representation of a transfer function
)(
)()(
1
1
i
n
i
i
m
i
ps
zssF
i
n
i
i
m
i
ps
zs
lengthspole
lengthszeroM
1
1
n
ii
m
ii pszs
anglespoleangleszero
11
)()(
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Vector s(s+a)
(s+a)(s+7)s = 5+j2
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Example
)2(
)1()(
ss
ssF
34.114217.0
04.1041787.1265
57.11620
)41)(43(
42
jj
j
Find F(s) at s = -3+j4
)2(
)1()(
ss
ssF
INC 341 PT & BP
What is root locus and why is it needed?
• Fact I: poles of closed-loop system are an important key to describe a performance of the system (transient response, i.e. peak time, %overshoot, rise time), and stability of the system.
• Fact II: closed-loop poles are changed when varying gain.
• Implication: Root locus = paths of closed-loop poles as gain is varied.
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Cameraman
Object Trackingusing infrared
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Varying gain (K)
Varying K, closed-loop poles are moving!!!
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Transient:• K<25 overdamped• K=25 critically damped• K>25 underdamped
• Settling time remains the same under underdamped responses.
Stability:• Root locus never crosses
over into the RHP, system is always stable.
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Concept of Root Locus
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)()(1
)()(
sHsKG
sKGsT
Characteristic equation
18011)()( sHsKG
Closed-loop transfer function
magnitude 1)()( sHsKG
,...3,2,1
180)12()()(
k
ksHsKG
phase
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magnitude 1)()( sHsKG
,...3,2,1
180)12()()(
k
ksHsKG phase
If there is any point on the root locus, its magnitude and phase will be consistant with the follows:
Note that: phase is an odd multiple of 180
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Example Is the point -2+3j a closed-loop pole for some value of gain? Or is the point on the root locus?
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55.7043.1089057.7131.564321
)2)(1(
)4)(3()()(
ss
ssKsHsKG
-2+3j is not on the root locus!!! What about ?)2/2(2 j
INC 341 PT & BP
)()(
1
1)()(
sHsGK
sHsKG
33.022.112.2
22.1707.021
43
LL
LLK
43
21)(LL
LLsG
The angles do add up to 180!!! is a point on the root locus )2/2(2 j
What is the corresponding K?
INC 341 PT & BPINC 341 PT & BP
Sketching Root Locus
1. Number of branches
2. Symmetry
3. Real-axis segment
4. Starting and ending points
5. Behavior at infinity
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1. Number of branchesNumber of branches = number of closed-loop poles
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2. SymmetryRoot locus is symmetrical about the real axis
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3. Real-axis segment
On the real axis, the root locus exists to the left of an odd number of real-axis
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180)12()()( ksHsKG
• Sum of angles on the real axis is either 0 or 180 (complex poles and zeroes give a zero contribution).
• Left hand side of even number of poles/zeros on the real axis give 180 (path of root locus)
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Example
root locus on the real axis
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4. Starting and ending points
Root locus starts at finite/infinite poles of G(s)H(s) And ends at finite/infinite zeros of G(s)H(s)
)()(1
)()(
sHsKG
sKGsT
closed-loop transfer function
)(
)()(
sD
sNsG
G
G )(
)()(
sD
sNsH
H
H
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)()()()(
)()()(
sNsKNsDsD
sDsKNsT
HGHG
HG
K=0 (beginning) poles of T(s) are
K=∞ (ending) poles of T(s) are
)()( sDsD HG
)()( sNsKN HG
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Example
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5. Behavior at infinity
Root locus approaches asymptote as the Locus approaches ∞, the asymptotes is given by
zeros finite#poles finite#
zeros finitepoles finite
a
...,2,1,0
zeros finite#poles finite#
)12(
k
ka
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)2)(1()()(
sss
KsHsKG
Rule of thumb
# of poles = # of zeroes
has 3 finite poles at 0 -1 -2, and 3 infinite zeroes at infinity
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Example
Sketch root locus
3
4
14
)3()421(0
2kfor , 3/5
1kfor ,
0kfor , 3/
zeros finite#poles finite#
)12(
k
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