chaos suppression and stabilization of generalized liu chaotic control system
DESCRIPTION
In this paper, the concept of generalized stabilization for nonlinear systems is introduced and the stabilization of the generalized Liu chaotic control system is explored. Based on the time domain approach with differential inequalities, a suitable control is presented such that the generalized stabilization for a class of Liu chaotic system can be achieved. Meanwhile, not only the guaranteed exponential convergence rate can be arbitrarily pre specified but also the critical time can be correctly estimated. Finally, some numerical simulations are given to demonstrate the feasibility and effectiveness of the obtained results. Yeong-Jeu Sun | Jer-Guang Hsieh "Chaos Suppression and Stabilization of Generalized Liu Chaotic Control System" Published in International Journal of Trend in Scientific Research and Development (ijtsrd), ISSN: 2456-6470, Volume-3 | Issue-1 , December 2018, URL: https://www.ijtsrd.com/papers/ijtsrd20195.pdf Paper URL: http://www.ijtsrd.com/engineering/electrical-engineering/20195/chaos-suppression-and-stabilization-of-generalized-liu-chaotic-control-system/yeong-jeu-sunTRANSCRIPT
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Chaos Suppression Generalized Liu Chaotic Control System
Yeong
Department of Electrical Engineering
ABSTRACT In this paper, the concept of generalized stabilization for nonlinear systems is introduced and the stabilization of the generalized Liu chaotic control system is explored. Based on the timeapproach with differential inequalities, a suitable control is presented such that the generalized stabilization for a class of Liu chaotic system can be achieved. Meanwhile, not only the guaranteed exponential convergence rate can be arbitrarily prespecified but also the critical time can be correctly estimated. Finally, some numerical simulations are given to demonstrate the feasibility and effectiveness of the obtained results. Key Words: Generalized synchronization, Liu chaotic system, critical time, exponential convergence rate 1. INTRODUCTION In recent years, chaotic dynamic systems have been widely investigated by researchers; see, for instance, [1-12] and the references therein. Very often, chaos in many dynamic systems is an origin of the generationof oscillation and an origin of instability. control system, it is important to design a controller that has both good transient and steady-state response.Furthermore, suppressing the occurrence of chaos plays an important role in the controller design of a nonlinear system. In the past decades, various methodologies in control design of chaotic system have been presentedvariable structure control approach, approach, adaptive control approach, adaptive sliding mode control approach, back stepping control approach, and others.
International Journal of Trend in Scientific Research and Development (IJTSRD)
International Open Access Journal | www.ijtsrd.com
ISSN No: 2456 - 6470 | Volume - 3 | Issue – 1 | Nov
www.ijtsrd.com | Volume – 3 | Issue – 1 | Nov-Dec 2018
Chaos Suppression and Stabilization of Generalized Liu Chaotic Control System
Yeong-Jeu Sun1, Jer-Guang Hsieh2 1Professor, 2Chair Professor
Electrical Engineering, I-Shou University, Kaohsiung
he concept of generalized stabilization for nonlinear systems is introduced and the stabilization of the generalized Liu chaotic control system is explored. Based on the time-domain approach with differential inequalities, a suitable
uch that the generalized stabilization for a class of Liu chaotic system can be achieved. Meanwhile, not only the guaranteed exponential convergence rate can be arbitrarily pre-specified but also the critical time can be correctly
numerical simulations are given to demonstrate the feasibility and effectiveness
Generalized synchronization, Liu chaotic system, critical time, exponential convergence rate
tic dynamic systems have been ; see, for instance,
] and the references therein. Very often, chaos in an origin of the generation
an origin of instability. For a chaotic control system, it is important to design a controller
state response. Furthermore, suppressing the occurrence of chaos
oller design of a
In the past decades, various methodologies in control presented, such as
time-domain approach, adaptive control approach, adaptive sliding
stepping control
In this paper, the concept of generalized for nonlinear dynamic systems is introduced and the stabilizability of generalized Liu chaotic system will be investigateddomain approach with differential inequality, a suitable control will be offered generalized stabilization can be achieved for a class of Liu chaotic system. Not only correctly estimated, but alsoexponential convergence rate can be arbitrarily prespecified. Several numerical simulations will also be provided to illustrate the use of the main results. The layout of the rest of this paper is organized as follows. The problem formulation, maicontroller design procedure are presentedNumerical simulations are given in Section 3 the effectiveness of the developed results.conclusion remarks are drawn 2. PROBLEM FORMULATION AND MAIN
RESULTS Nomenclature
nℜ the n-dimensional real spacea the modulus of a complex number
TA the transport of the matrix x the Euclidean norm of the vector
In this paper, we explore the following generalized Liu chaotic system:
( ) ( ) ( ) ( ),122111 tutxatxatx ++=& ( ) ( ) ( ) ( ) ( ),2314132 tutxtxatxatx ++=& ( ) ( ) ( ) ( )
( ) ( ) ,0,3218
3726153
≥∀++
++=
ttutxa
txatxatxatx&
Research and Development (IJTSRD)
www.ijtsrd.com
1 | Nov – Dec 2018
Dec 2018 Page: 1112
f Generalized Liu Chaotic Control System
Kaohsiung, Taiwan
generalized stabilizability dynamic systems is introduced and the
generalized Liu chaotic control investigated. Based on the time-
domain approach with differential inequality, a offered such that the
stabilization can be achieved for a class of system. Not only the critical time can be
, but also the guaranteed exponential convergence rate can be arbitrarily pre-
. Several numerical simulations will also be provided to illustrate the use of the main results.
The layout of the rest of this paper is organized as The problem formulation, main result, and
controller design procedure are presented in Section 2. given in Section 3 to show developed results. Finally,
in Section 4.
ROBLEM FORMULATION AND MAIN
dimensional real space the modulus of a complex number a
the transport of the matrix A the Euclidean norm of the vector nx ℜ∈
the following generalized
(1a) (1b)
(1c)
International Journal of Trend in Scientific Research and Development (IJTSRD) ISSN: 2456
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( ) ( ) ( )[ ][ ] ,
000
302010
321
T
T
xxx
xxx
=
where ( ) ( ) ( ) ( )[ ] 3
321: ℜ∈= Ttxtxtxtx is the state vector,
( ) ( ) ( ) ( )[ ] 3321: ℜ∈= Ttutututu is the system
[ ]Txxx 302010 is the initial value, and ai ,
the parameters of the system. The original system is a special case of system (1) with
1021 =−= aa , ,403 =a ,14 −=a ,065 == aa
48 =a . It is well known that the system (1) without any control (i.e., ( ) 0=tu ) displays chaotic behavior for certain values of the parameters [1]. The paper is to search a novel control for the system (1) such that the generalized stability of the controlled system can be guaranteed. In this concept of generalized stabilization will be introduced. Motivated by time-domain approach with differential inequality, a suitable control be established. Our goal is to design a control such that the generalized stabilization of systemachieved. Let us introduce a definition which will be used in subsequent main results. 1 There exist two positive numbers k
that ( ) 0, ≥∀⋅≤ − tektx tb .
2 There exists a positive number ( ) ctttx ≥∀= ,0 .
Definition 1 The system (1) is said to realize the stabilization, provided that there exist a suitable control u such that the conditons (i) and (ii) are satisfied. In this case, the positive number the exponential convergence rate and number ct is called the critical time. Now we present the main result for the stabilization of the system (1) via approach with differential inequalities. Theorem 1 The system (1) realizes the generalized under the following control
( ) ( ) ( ) ( ) ( ),12122111 taxtxatxbatu −−−+−= α (2a)
( ) ( ) ( ) ( ) ( )( ),12
2
2314132
tax
tbxtxtxatxatu−−
−−−=α (2b)
( ) ( ) ( ) ( ) ( )( ) ( ),12
3218
3726153
taxtxa
txbatxatxatu−−−
+−−−=α (2c)
of Trend in Scientific Research and Development (IJTSRD) ISSN: 2456
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(1d)
is the state vector,
is the system control,
ℜ∈b, indicate . The original Liu chaotic
is a special case of system (1) with ( ) ,0=tu 5.27 −=a , and
It is well known that the system (1) without ) displays chaotic behavior for
he aim of this for the system (1) of the feedback-In this paper, the
stabilization will be domain approach with
suitable control strategy will a control such
stabilization of system (1) can be
Let us introduce a definition which will be used in
k and b , such
There exists a positive number ct such that
The system (1) is said to realize the generalized there exist a suitable
such that the conditons (i) and (ii) are In this case, the positive number b is called
convergence rate and the positive
the generalized (1) via time-domain
generalized stabilization
where ,0,0 >> ba12
1:
−−+=
p
qpα , with
In this case, the pre-convergence rate and the guaranteed critical timegiven by b and
( ) ( )[( )12
00ln
23
22
21
b
xxx
b
a
tc α−−
++=
respectively Proof. From (1)-(2), the feedbackcan be performed
( ) ,12111
−−−= αxabxx&
( ) ,12222
−−−= αxabxx&
( ) ,12333
−−−= αxabxx& Let
( )( ) ( ) ( )txtxtxW T= . The time derivative of ( )( )txW feedback-controlled system is given by
2211 22 xxxxW &&& ⋅+⋅= α2
122
21 2222 axaxbxb −⋅−⋅−⋅−=
( )αα 22
2122 xxaWb +−⋅−=
.0,22 ≥∀⋅−⋅−≤ tWaWb α It follows that ( ) ( )
( ) .0,12
121 1
≥∀−−≤−+− −−
ta
bWWW
ααα αα &
Define
( ) ( )( ) .0,: 1 ≥∀= − ttxWtQ α From (6) and (7), it can be readily obtained that
( ) ( ),1212 ≥∀−−≤−+ tabQQ αα&
It is easy to deduce that
( ) ( ) ( ) ( ) (( ) ( )[ ]
( ) ( ) .0,12
12
12
12
1212
≥∀−−≤
⋅=
−⋅+⋅
−
−
−−
tea
tQedt
d
QbetQe
bt
bt
btbt
α
α
αα
α
α&
It follows that
( ) ( )[ ]( ) ( ) ( )012
0
12
QtQe
dttQedt
d
bt
tbt
−⋅=
⋅
−
−∫
α
α
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, with Nqp ∈, and qp >
-specified exponential guaranteed critical time are
( )]) ,
012
3
bb
aα
+−
(3)
feedback-controlled system
(4a)
(4a)
(4a)
(5)
along the trajectories of is given by
α22xa ⋅
(6)
(7)
), it can be readily obtained that .0
( )t
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( ) ( )
( )( ) .0,1
12
12
0
12
≥∀−−=
−−≤
−
−∫
teb
a
dtea
bt
tbt
α
αα
Consequently, we have
( ) ( ) ( )
.0
,0 12
≥∀
−⋅
+≤ −−
t
b
ae
b
aQtQ btα
(8)
Hence, from (6), (7), and (8), we have (i) If ,0 ctt ≤≤
( )( ) ( ) ( )( )
;011
1222α
αα−
−−−
−⋅
+≤b
ae
b
axtxW bt (ii) If
( ) 0=tx . Consquently, we conclude that (i) If ,0 ctt ≤≤
( ) ( )( )
;0221
22 bteb
axtx −
−− ⋅
+≤α
α
(ii) If ,ctt ≥ ( ) ,0=tx in view of (5) with above condition (i)completes the proof. □ 3. NUMERICAL SIMULATIONS Consider the generalized Liu chaotic systemwith 1021 =−= aa , ,403 =a ,14 −=a 5 = aa
, ,48 =a and ( ) [ ]Tx 2240 −= . Our objective, inexample, is to design a feedback control such that the system (1) realize the generalized stabilizationwith the guaranteed exponential convergence rate
5.0=b . From (2), with ,3,100 === qpa
8.0=α , ( ) ( ) ( ) ( ),100105.10 6.0
1211 txtxtxtu −+−= (9a) ( ) ( ) ( ) ( ) ( )
( ),100
5.0406.0
2
23112
tx
txtxtxtxtu
−
−+−= (9b)
( ) ( ) ( ) ( ),10042 6.03
2133 txtxtxtu −−= (9c)
Consequently, by Theorem 1, we conclude that system (1) achieves generalized stabilization parameters of 1021 =−= aa , ,403 =a 4 =a
5.27 −=a , 48 =a , and feedback control law of (Furthermore, the exponential convergence rateguaranteed critical time are given by
047.0=ct . The typical state trajectories of uncontrolled systems and controlled systems are depicted in FigFigure 2, respectively. From the foregoing simulations
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(ii) If ,ctt ≥
with above condition (i). This
Liu chaotic system of (1) ,06 =a 5.27 −=a
Our objective, in this example, is to design a feedback control such that the
stabilization with with the guaranteed exponential convergence rate
,2 we deduce
, we conclude that the achieves generalized stabilization with
,1− ,065 == aa feedback control law of (9).
exponential convergence rate and the iven by 5.0=b and
of uncontrolled systems and controlled systems are depicted in Figure 1 and
, respectively. From the foregoing simulations
results, it is seen that the dynamic system of (achieves the generalized stabilization under the control law of (9). 4. CONCLUSION In this paper, the concept of generalizedfor nonlinear systems has been introduced and the stabilization of generalized Liu chaotic has been studied. Based on the timewith differential inequalities, a sbeen presented such that the generalized for a class of Liu chaotic system Besides, not only the guaranteed exponential convergence rate can be arbitrarily prealso the critical time can be correctly estimated.Finally, some numerical simulations have been offered to show the feasibility and effectiveness of the obtained results. ACKNOWLEDGEMENT The authors thank the Ministry of Science and Technology of Republic of China for supporting this work under grants MOST 106MOST 106-2813-C-214-025-EE-214-030. REFERENCES 1. D. Su, W. Bao, J. Liu, and
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of Trend in Scientific Research and Development (IJTSRD) ISSN: 2456-6470
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Liu chaotic system can be achieved. Besides, not only the guaranteed exponential convergence rate can be arbitrarily pre-specified but
itical time can be correctly estimated. Finally, some numerical simulations have been offered to show the feasibility and effectiveness of the
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Figure 1: Typical state trajectories of the system (1) with ,0=u 1021 =−= aa , 3 =a
5.27 −=a , and
Figure 2: Typical state trajectories of the feedbackcontrolled system of (
0 5 10 15 20 25-40
-20
0
20
40
60
80
100
120
t (sec)
x1(t
); x
2(t)
; x3
(t)
x1: the Blue Curve x2: the Green Curve
0 0.01 0.02 0.03 0.04-2
-1
0
1
2
3
4
t (sec)
x1(t
); x
2(t)
; x3
(t)
x1
x2
x3
of Trend in Scientific Research and Development (IJTSRD) ISSN: 2456-6470
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Typical state trajectories of the system (1)
,40 ,14 −=a ,065 == aa and 48 =a .
Typical state trajectories of the feedback-
controlled system of (1) with (9).
30 35 40 45 50
x2: the Green Curve x3: the Red Curve
0.05 0.06 0.07 0.08