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Lecture introduction to control systems chapter 5 analysis of control system performance (dr huynh thai hoang)

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Tiêu đề Analysis Of Control System Performance
Người hướng dẫn Dr. Huynh Thai Hoang
Trường học Ho Chi Minh City University of Technology
Chuyên ngành Automatic Control
Thể loại Lecture Notes
Năm xuất bản 2011
Thành phố Ho Chi Minh City
Định dạng
Số trang 41
Dung lượng 514,76 KB

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First--order system order system The relationship between the pole and the time response æ The further the pole of the system is from the imaginary axis, thesmaller the time constant and

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Lecture Notes

Introduction to Control Systems

Instructor: Dr Huynh Thai Hoang Department of Automatic Control Faculty of Electrical & Electronics Engineering

Ho Chi Minh City University of Technology

Email: hthoang@hcmut.edu.vn

huynhthaihoang@yahoo.com Homepage: www4.hcmut.edu.vn/~hthoang/

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Chapter 5

ANALYSIS OF CONTROL SYSTEM

PERFORMANCE

Trang 3

æ The optimal performance index

æ Relationship between frequency domain performances and time

domain performances

Trang 4

Performance criteria

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Performance criteria: Steady state error

()

(t r t y t

e = − fbE(s) = R(s) −Y fb(s)

æ Steady-state error: is the error when time approaching infinity

)(

Trang 6

æ Overshoot: refers to an output exceeding its steady state value

Performance criteria

Performance criteria – – Percent of Overshoot (POT) Percent of Overshoot (POT)

æ Overshoot: refers to an output exceeding its steady-state value.

POT

ss

y

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æ S ttli ti (t ) i th ti i d f th f t t

Performance criteria

Performance criteria – – Settling time and rise time Settling time and rise time

æ Settling time (t s): is the time required for the response of a system toreach and stay within a range about the steady-state value of sizespecified by absolute percentage of the steady-state value (usually2% or 5%)

æ Rise time (t r): is the time required for the response of a system torise from 10% to 90% of its steady-state value

rise from 10% to 90% of its steady state value

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Steady Steady state error state error

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()

(

s H s G

s

R s

)

(lim

)(

sE

e

s s

ss = → = → +

æ Steady-state error:

)()(1

Trang 10

G(s)H(s) does not have

any deal integral factor

G(s)H(s) has at least 1 ideal integral factor

Trang 11

G(s)H(s) does not have

deal integral factor

G(s)H(s) has 1 ideal integral factor

G(s)H(s) has at least 2 ideal integral factors

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G(s)H(s) has less than 2

ideal integral factors

G(s)H(s) has 2 ideal integral factors

G(s)H(s) has more than 2 ideal integral factors

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Transient response

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1

)(

1)

()()

s G s R s

Y

1

+

Ts s

e K

t

Trang 15

Pole – zero plot

of a first order system

Transient response

of the first order

)1

()

(t K e t / T

y(t) = K(1 e− )

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First order system order system – – Remarks Remarks

æ First order system has only one real pole at (−1/T), its transientresponse doesn’t have overshoot

æ Time constant T: is the time required for the step response of the

system to reach 63% its steady-state value

æ The further the pole ( 1/T) of the system is from the imaginary

æ The further the pole (−1/T) of the system is from the imaginaryaxis, the smaller the time constant and the faster the time response

where ε = 0 02 (2% criterion) or ε = 0 05 (5% criterion)

where ε 0.02 (2% criterion) or ε 0.05 (5% criterion)

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First order system order system

The relationship between the pole and the time response

æ The further the pole of the system is from the imaginary axis, thesmaller the time constant and the faster the time response of the

Pole – zero plot

of a first order system

Transient response

of the first order

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Second order oscillating system order oscillating system

12

æ The transfer function of the second-order oscillating system:

1 ( ω = < ξ <

æ The system has two complex conjugate poles:

2 2

2 2

2 1

2

) (

n

n s s

Ts s

T

s G

ω ξω

( ) ( )

2 2

( ) ( )

(

n

n s s

s

s G s R s

Y

ω

ξω + +

t

n

) 1

( sin 1

1

1 )

(

Trang 19

Pole – zero plot of a second

order oscillating system

Trang 20

Second order oscillating system order oscillating system – – Remark Remark

æ A second order oscillation system has two conjugated complex

æ A second order oscillation system has two conjugated complex

poles, its transient response is a oscillation signal

ξ , ( the closer the poles are to

the real axis ) the faster the

response decays.

ξ = 0.6

response decays.

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Second order oscillating system order oscillating system – – Overshoot Overshoot

æ Transient response of the second order oscillating system has

% 100

The percentage of overshoot:

Ø The larger the value ξ, (the closer the poles are to the real axis) the smaller the

POT

Ø The smaller the value ξ,

(the closer the poles are to

(the closer the poles are to the imaginary axis) the larger the POT

ξ

The relationshipThe relationship

between POT and ξ

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Second order oscillating system order oscillating system

Relationship between pole location and transient response

æ The second order systems that have the poles located in the same

rays starting from the origin have the same damping constant, then

cosθ = ξ

Pole – zero plot of a second Transient response of a second

t

0Pole zero plot of a second

order oscillating system

Transient response of a second order oscillating system

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Second order oscillating system order oscillating system

Relationship between pole location and transient response (cont’)

æ The second order systems that have the poles located in the same

distance from the origin have the same natural oscillation

Pole zero plot of a second

order oscillating system

Transient response of a second order oscillating system

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Second order oscillating system order oscillating system

Relationship between pole location and transient response (cont’)

Pole zero plot of a second

order oscillating system

Transient response of a second order oscillating system

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Transient response of high order system

æ High order systems are the system that have more than 2 poles

æ High-order systems are the system that have more than 2 poles

æ If a high order system have a pair of poles located closer to the

imaginary axis than the others then the high order system can beapproximated to a second order system The pair of poles nearest tothe imaginary axis are called the dominant poles

A high order system can be approximated

by a dominated-pole second order systems

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Performance indices

Trang 28

Integral performance indices

)

( dt t e

2

)

( dt t e

t

J ITAE

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Optimum systems

æ A control system is optimum when the selected performance index is

æ A control system is optimum when the selected performance index is

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ITAE optimal control

æ ITAE is usually used in design of control system

æ ITAE is usually used in design of control system

æ An n-order system is optimal according to ITAE criterion if thedenominator of its transfer function has the form:

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ITAE optimal control (cont’)

æ Optimal response according to ITAE criterion

æ Optimal response according to ITAE criterion

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Relationship between frequency domain p p q q y y

performances and time domain performances

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Relationship between frequency response and steady state error

) (

lim )

( ) (

lim

0

ω G j H j s

H s G

K

s

p = → = →

) (

) (

lim )

( ) (

lim

0

ω j G j H j s

H s G s

K

s

v = → = →

) (

) (

) (

lim )

( ) (

K

s

a = → = →

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Relationship between frequency response and steady state error

æ Steady state error of the closed loop system depends on the

æ Steady state error of the closed-loop system depends on the

magnitude response of the open-loop system at low frequencies butnot at high frequencies

æ The higher the magnitude response of the open-loop system at low

frequencies, the smaller the steady-state error of the closed-loop

s stem

system

æ In particular, if the magnitude response of the open-loop system isinfinity as frequency approaching zero, then the steady-state error ofy q y pp g , ythe closed-loop system to step input is zero

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Relationship between frequency response and transient response

æ In the frequency range ω <ω because G( jω) >1 then:

æ In the frequency range ω <ωc, because G( jω) >1 then:

1)

(

)(

)(

1

)

()

ω ω

j G

j G j

G

j

G j

G cl

)(

)( jω G jω

G

æ In the frequency range ω >ωc, because G( jω) <1 then:

)(

)( jω G jω

G

⇒ Bandwidth of the closed loop system is approximate the gain

)

(1

)(

)(

1

)

()

j

G j

+

=

⇒ Bandwidth of the closed-loop system is approximate the gain

crossover frequency of the open-loop system

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Relationship between frequency response and transient response

closed-loop system

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Relationship between frequency response and transient response

æ The higher the gain crossover frequency of open loop system the

æ The higher the gain crossover frequency of open-loop system, the

wider the bandwidth of closed-loop system ⇒ the faster the

response of close-loop system, the shorter the settling time

c

qd c

t

ω

π ω

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Example of relationship between gain crossover frequency and settling time

) 1 08

0 )(

1 1

0 (

10 )

(

+ +

=

s s

s

s G

0 )(

1 1

0

s

Trang 39

Example of relationship between gain crossover frequency and settling time

0 (

50 )

(

+

=

s s

s

G

) 1 1

0 ( s +

s

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Example of relationship between phase margin and POT

) 1 08

0 )(

1 1

0 (

6 )

(

+ +

=

s s

s

s G

0 )(

1 1

0

s

Trang 41

Example of relationship between phase margin and POT (cont’)

) 1 1

0 (

6 )

(

+

=

s s

s G

0 ( s +

s

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