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Lypunov Stability
By :
Rajasekhar
Sahin P
2
Stability
• Asymptotically stable
– Consider a system represent in state space:
• Bounded-Input Bounde-Output stable
– (Input-output stability)
∞→→
==
tastxif
xxAxx
0)(
)0( 0

∞<≤→∞<≤ MtyNtu )()(
for all bounded input
3
Stability condition
• Asymptotically stable
• All the eigenvalues of the system have
negative real parts (i.e. in the LHP)
• BIBO stable
• All the transfer function poles be in the
LHP
4
Lyapunov stability
A state of an autonomous system is called an equilibrium
state, if starting at that state the system will not move from it in
the absence of the forcing input.
ex
)),(),(( ttutxfx = 0,0),0,( tttxf e ≥=
)(
1
1
32
10
tuxx 





+





−−
=






=





⇒=











−−
=
0
0
0
32
10
0)(
2
1
2
1
e
e
e
e
x
x
x
x
tulet
example
1x
2x
Equilibrium point
5
)(
1
2
20
00
tuxx 





+





−
=






=





⇒=











−
=
0
0
20
00
0)(
2
1
2
1 k
x
x
x
x
tulet
e
e
e
e
example
1x
2x
Equilibrium line
6
Definition: An equilibrium state of an autonomous system is
stable in the sense of Lyapunov if for every , exist a
such that for
ex
0ε 0)( εδ
εδ  ee xxtxxx −⇒− ),( 00 0tt ≥∀
δ
ε
1x
2x
ex
0x
7
Definition: An equilibrium state of an autonomous system is
asymptotically stable if
(i) It is stable and
(ii) exist if
ex
→aδ ∞→→−⇒− tasxtxxx eae ,0)(0 δ
δ
ε
1x
2x
ex
0x
aδ
8
Asymptotically stable in the large
( globally asymptotically stable)
(1) If the system is asymptotically stable for all the initial states
.
(2) The equilibrium point is said to be asymptotically or
exponentially stable in the large .
(3) It is also called globally asymptotically stable.
)( 0tx
9
10
11
13
A scalar function V(x) is positive (negative) semidefinite if
(i) V(0)=0 and V(x)=0 possibly at some
(ii)
0≠x
)0(0)( ≤≥xV
Lyapunov’s function
A function V(x) is called a Lyapunov function if
(i) V(x) and are continuous in a region R containing the
origin (E.S.)
(ii) V(x) is positive definite in R.
(iii) relative to a system along the trajectory of
the system is negative semi-definite in R.
ix
xv
∂
∂ )(
)(xfx = )(xV
A scalar function V(x) is positive (negative) definite if
(i) V(0)=0
(ii) V(x)>0 (<0) for 0≠x
14
A function is not definite or semidefinite in either sense
is defined to be indefinite.
example
2
3
2
2
2
213211
2
321
2
2
2
13211
)(),,(
22),,(
xxxxxxxV
xxxxxxxxV
+++=
+++=
positive definite
2
3
4
2
4
13212 ),,( xxxxxxV ++= positive definite
)3(),,(
3),,(
2
3
2
3
2
2
2
13213
4
3
2
3
2
2
2
13213
xxxxxxxV
xxxxxxxV
−++=
−++=
3
3
3
3
≤xif
xif  p.d.
p.s.d.
15
2
3
2
213214 )(),,( xxxxxxV ++= p.s.d.
2
3213215 ),,( xxxxxxV ++= indefinite
Quadratic form
[ ]
AXX
x
x
x
aaa
a
aaa
xxx
xxaxV
T
nnnnn
n
n
ji
n
i
n
j
ij
∆
= =
=
























=
= ∑∑




 2
1
21
21
11211
21
1 1
)(
16


















++
+
++
⇒












nnnnnn
nn
nnnn
n
aaaaa
aa
aaaaa
aaa
a
aaa






)(
2
1
)(
2
1
)(
2
1
)(
2
1
)(
2
1
2211
2112
11211211
21
21
11211
Symmetry
matrix Q
)(
2
1 T
AAQ +=
17
Q: symmetric matrix then
(1) Q is p.d. V(x) is p.d.
(2)Q is n.d. V(x) is n.d.
(3)Q is p.s.d. V(x) is p.s.d.
(4)Q is n.s..d. V(x) is n.s..d.
(5)Q is indefinite. V(x) is indefinite.
(6) Q is p.d. eigenvalues of Q are positives
(7) Q is n.d. eigenvalues of Q are negatives
QxxxV T
=)(
18
Sylvester’s criterion
A symmetric matrix Q is p.d. if and only if all its n
leading principle minors are positive.
nn×
Definition
The i-th leading principle minor of an
matrix Q is the determinant of the matrix extracted from
the upper left-hand corner of Q.
niQi ,,3,2,1 = nn×
ii×
QQ
qq
qq
Q
qQ
qqq
qqq
qqq
Q
==
=










=
3
2221
2111
2
111
333231
232221
131211
19
Remark
(1) are all negative Q is n.d.
(2) All leading principle minors of –Q are positive Q is n.d.
nQQQ ,, 21
example
[ ]
[ ]




















=




















=
++++=
3
2
1
321
3
2
1
321
2
332
2
131
2
1
132
330
202
100
630
402
6342)(
x
x
x
xxx
x
x
x
xxx
xxxxxxxxV
024
06
02
3
2
1



−=
=
=
Q
Q
Q
Q is not p.d.
20
Lyapunov’s method
Consider the system
If in a neighborhood R about the origin a Lyapunov
function V(x) can be found such that is n.d. along the
trajectory then the origin is asymptotically stable.
)(xV
0)0(),( == fxfx
Consider linear autonomous system
0≠= AifAxx ..0 SEx ⇒=
pxxxV T
=)(Let Lyapunov function
Qxx
xPAPAx
PAxxPxAx
xPxPxxxV
T
TT
TTT
TT
−=
+=
+=
+=⇒
)(
)( 
)( PAPAQ T
+−=
If Q is p.d. then is n.d.)(xV
0=x is asymptotically stable
21
example
xx 





−−
=
11
10
 0.. =⇒ xSE






=





=






−
−
=





−−





+











−
−
−=+
=
21
13
2
1
10
01
11
10
11
10
2212
1211
2212
1211
2212
1211
pp
pp
P
pp
pp
pp
pp
IPAPA
IQlet
T
050311  == Pp P is p.d.
System is asymptotically stable
The Lyapunov function is:
)()(
)223(
2
1)(
2
2
2
1
2
221
2
1
xxxV
xxxxPxxxV T
+−=
++==


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Lyapunov stability

  • 2. 2 Stability • Asymptotically stable – Consider a system represent in state space: • Bounded-Input Bounde-Output stable – (Input-output stability) ∞→→ == tastxif xxAxx 0)( )0( 0  ∞<≤→∞<≤ MtyNtu )()( for all bounded input
  • 3. 3 Stability condition • Asymptotically stable • All the eigenvalues of the system have negative real parts (i.e. in the LHP) • BIBO stable • All the transfer function poles be in the LHP
  • 4. 4 Lyapunov stability A state of an autonomous system is called an equilibrium state, if starting at that state the system will not move from it in the absence of the forcing input. ex )),(),(( ttutxfx = 0,0),0,( tttxf e ≥= )( 1 1 32 10 tuxx       +      −− =       =      ⇒=            −− = 0 0 0 32 10 0)( 2 1 2 1 e e e e x x x x tulet example 1x 2x Equilibrium point
  • 6. 6 Definition: An equilibrium state of an autonomous system is stable in the sense of Lyapunov if for every , exist a such that for ex 0ε 0)( εδ εδ  ee xxtxxx −⇒− ),( 00 0tt ≥∀ δ ε 1x 2x ex 0x
  • 7. 7 Definition: An equilibrium state of an autonomous system is asymptotically stable if (i) It is stable and (ii) exist if ex →aδ ∞→→−⇒− tasxtxxx eae ,0)(0 δ δ ε 1x 2x ex 0x aδ
  • 8. 8 Asymptotically stable in the large ( globally asymptotically stable) (1) If the system is asymptotically stable for all the initial states . (2) The equilibrium point is said to be asymptotically or exponentially stable in the large . (3) It is also called globally asymptotically stable. )( 0tx
  • 9. 9
  • 10. 10
  • 11. 11
  • 12. 13 A scalar function V(x) is positive (negative) semidefinite if (i) V(0)=0 and V(x)=0 possibly at some (ii) 0≠x )0(0)( ≤≥xV Lyapunov’s function A function V(x) is called a Lyapunov function if (i) V(x) and are continuous in a region R containing the origin (E.S.) (ii) V(x) is positive definite in R. (iii) relative to a system along the trajectory of the system is negative semi-definite in R. ix xv ∂ ∂ )( )(xfx = )(xV A scalar function V(x) is positive (negative) definite if (i) V(0)=0 (ii) V(x)>0 (<0) for 0≠x
  • 13. 14 A function is not definite or semidefinite in either sense is defined to be indefinite. example 2 3 2 2 2 213211 2 321 2 2 2 13211 )(),,( 22),,( xxxxxxxV xxxxxxxxV +++= +++= positive definite 2 3 4 2 4 13212 ),,( xxxxxxV ++= positive definite )3(),,( 3),,( 2 3 2 3 2 2 2 13213 4 3 2 3 2 2 2 13213 xxxxxxxV xxxxxxxV −++= −++= 3 3 3 3 ≤xif xif  p.d. p.s.d.
  • 14. 15 2 3 2 213214 )(),,( xxxxxxV ++= p.s.d. 2 3213215 ),,( xxxxxxV ++= indefinite Quadratic form [ ] AXX x x x aaa a aaa xxx xxaxV T nnnnn n n ji n i n j ij ∆ = = =                         = = ∑∑      2 1 21 21 11211 21 1 1 )(
  • 16. 17 Q: symmetric matrix then (1) Q is p.d. V(x) is p.d. (2)Q is n.d. V(x) is n.d. (3)Q is p.s.d. V(x) is p.s.d. (4)Q is n.s..d. V(x) is n.s..d. (5)Q is indefinite. V(x) is indefinite. (6) Q is p.d. eigenvalues of Q are positives (7) Q is n.d. eigenvalues of Q are negatives QxxxV T =)(
  • 17. 18 Sylvester’s criterion A symmetric matrix Q is p.d. if and only if all its n leading principle minors are positive. nn× Definition The i-th leading principle minor of an matrix Q is the determinant of the matrix extracted from the upper left-hand corner of Q. niQi ,,3,2,1 = nn× ii× QQ qq qq Q qQ qqq qqq qqq Q == =           = 3 2221 2111 2 111 333231 232221 131211
  • 18. 19 Remark (1) are all negative Q is n.d. (2) All leading principle minors of –Q are positive Q is n.d. nQQQ ,, 21 example [ ] [ ]                     =                     = ++++= 3 2 1 321 3 2 1 321 2 332 2 131 2 1 132 330 202 100 630 402 6342)( x x x xxx x x x xxx xxxxxxxxV 024 06 02 3 2 1    −= = = Q Q Q Q is not p.d.
  • 19. 20 Lyapunov’s method Consider the system If in a neighborhood R about the origin a Lyapunov function V(x) can be found such that is n.d. along the trajectory then the origin is asymptotically stable. )(xV 0)0(),( == fxfx Consider linear autonomous system 0≠= AifAxx ..0 SEx ⇒= pxxxV T =)(Let Lyapunov function Qxx xPAPAx PAxxPxAx xPxPxxxV T TT TTT TT −= += += +=⇒ )( )(  )( PAPAQ T +−= If Q is p.d. then is n.d.)(xV 0=x is asymptotically stable
  • 20. 21 example xx       −− = 11 10  0.. =⇒ xSE       =      =       − − =      −−      +            − − −=+ = 21 13 2 1 10 01 11 10 11 10 2212 1211 2212 1211 2212 1211 pp pp P pp pp pp pp IPAPA IQlet T 050311  == Pp P is p.d. System is asymptotically stable The Lyapunov function is: )()( )223( 2 1)( 2 2 2 1 2 221 2 1 xxxV xxxxPxxxV T +−= ++== 