VOL. 17 NO. (1994) 103-112
SOLUTIONS TO LYAPUNOV STABILITY PROBLEMS OF SETS:
NONLINEAR SYSTEMS WITH DIFFERENTIABLE MOTIONS
LJUBOMIR T.
GRUJI(
Department
of ElectricalEngineering UniversityofNatalRm.
1-05, Elec.Eng.
Bldg.King
George V Avenue,
Durban 4001, SouthAfrica(Received January
23,1991and in revisedform April 28,1993)
Abstract. Time-invariant nonlinearsystemswith differentiable motions are considered. The algorithmic necessaryand sufficient conditions are established in various forms for one-shot construction of a
Lyapunov
function, forasymptotic stabilityof acompactinvariant setandfor theexactdetermination of theasymptotic stabilitydomainofthe invariantset.
Theclassical conditionsareexpressedin terms of existenceof asystem
Lyapunov
functions. The conditions of theoremspresentedherein areexpressedviapropertiesof the solution vto-p,
orof the solutionwto-(1 w)p,
forarbitrarilyselectedp C.P(S ;f)
orp C.Pt(S ;f),
where familiesP(S;f)
andPt(S;f)
arewelldefined. The equation -p,or itsequivalent/,-(1 w)p,
should be solvedonlyfor oneselection of the functionp.
Key
Words and Phrases: NonlinearSystems, Lyapunov
Functions,andasymptotic stability.1991MathematicsSubjectClassificationCodes: 34A34, 93D05, 93D20.
1.
INTRODUCTION
The fundamentalclassicalproblemof the
Lyapunov
stability theory[5]
has beenthatofthe exactone-shot construction of asystem
Lyapunov
function. This is aconsequence
of the conditions forasymptotic stabilitybecausetheyareexpressed
fornonlinearsystemsvia existence6f
aLyapunov
function. Such classicalcriteriafor asymptotic stability ofasetwereproved
by Zubov[7,
p.204],
BhatiaandSztige [1,
p.207],
andLa
Salle[4, p. 32].
The
open
problemsare thefollowing:Whatare the
necessary
andsufficient conditionsforasymptotic
stability ofacompact
invariantsetJ,
which arenotexpressedvia existenceof aLyapunov
function?What are the necessary and sufficient conditions for one-shot algorithmic construction ofa
Lyapunov
function?Whatarethe
necessary
and sufficient conditionsforexactone-shot determinationoftheasymptotic stabilitydomain ofthe setJ?
The notion of the asymptotic stabilitydomain is defined inthe Appendix by following[2], [3].
All threeproblemsare solved in various forms in what follows for alargeclassof time-invariant nonlinearsystems.
2.
NOTATION
Capital
Roman
letterswilldenotesetsandspaces.J
will be an invariantsetof asystem,J CR’. Its
neighborhoodwillbe denotedby A(J),N(J)
orS(J),
and its6-neighborhoodwillbedesignated byB6(J), Bt(J)- {x "p(x,J) <. 6},
wherep(x,J)-inf{llx -yil "Y J}
withIlxll -(:x) .
Notice thatJCA(J)
and
J
CBn(J).
The closure, interior andboundaryofat J
aredenotedbyJ’, j
and&/. TheemptysetisO.
Ds(J),D,(J)
andD(J)
willbe usedfor the domain ofstabilityofJ,
the domain of attraction ofJ
and the domainof asymptotic stabilityofJ,
respectively.Their definitions aregivenin theAppendix
by referring to[21, 13].
A
motion.of thesystem tobe considered isdenotedbyx_..(t;x0)
withx_..(0;x0)- Xo.
Ifv:R" R
is differentiable thendv(x)/dt O(x)
istheEulefian
derivativeofvalongsystem motions.Other notation will be explained in thesequel.
SYSTEM DESCRIPTION
A
systemtobe studied is describedby--- f(x), (3.1a)
tR, xR’, f:R’--,R’. (3.1b)
Itisacceptedthat the systempossessesoneof thenext twosmoothnessproperties.
WeakSmoothness
Property:
(i) There is an
open
neighborhoodS(J)
of acompactinvariantsetJ
of thesystem(3. lab)
such that forevery
x0IS (J) -) ]:
(a)
thesystemhas theuniquesolutionx_.(t;x0),
and(b)
the motionx_(t;xo)
is defined, continuous and differentiable in(t,x6)Iox[S(J)-)],
1o lo(xo)
_CR+
and1o .
(ii)
For every
x0JR" -S(J)] every
motionx(t;Xo)
of thesystem(3. lab)
is continuousinStrong
SmoothnessProperty:
(i)
The system(3.1ab) possesses
the Weak SmoothnessProperty.
(ii) Iftheboundary
dS(J) orS(J)
isnon-emptythenevery
motionofthesystem(3. lab)
passingthrough
xo dS(J)
obeysinf{p[x_(t;xo),S(J)]:t R/}
>0 forevery xo #S(J).
4.
LYAPUNOV FUNCTION GENERATION AND DE’rERMINATION OF THE ASYMPTOTIC STABILITY DOMAIN FOR THE SYSTEM WITH STRONG SMOOTHNESS PROPERTY
A
function v"R" R
will be calledpositivedefinite
with respecttoJ
if and only ifthere is aneighborhood
A (J)
ofJ
such that (i)v(x)
is continuous inxE A (J), (ii) v(x
>O
forevery
x[A (J J ],
(iii)v(x)
0 foreveryx.
A
functionvispositivedefinite
onN(J)
with respecttoJ
if andonly
if theprecedingconditions(i)-(iii)
holdforA (J) N(J).
We
shall writeA, B.), D(.), N
andSinsteadofA(J), B(.)(J), D+)(J), N(J)
andS(J),
respectively, as soon asJ
isknown and fixed.In
thesequelthesetJ
isassumedknown and fixed.In
ordertogenerateav-function(Lyapunov function)
for thesystem(3.lab)
thefollowingdefinition isintroduced.Definition
1. (i)P(S;f)
isthefamilyof all functionsp:R" R
obeying1)-3), 1)
pisdifferentiable onS
andpositivedefinite onS
withrespecttoJ,
2)
forany
ct>Osuch thatB
CS
there is[A
>O, [A l?,(ct;p ;S ),
satisfyinginf[p(x
x(S B,)] [%
3)
thereisIx ]0, +oo[,Ix. Ix(o;/],
such thatthere existsasolutionv tothefollowing systemdetermined alongmotions of thesystem(3.lab),
d
v(x) [grad v(x)f(x) -p(x) (4.1a)
dt
v(x)-O, Yx
j(4.t,)
which isdefinedand continuous in x
E B,.
(ii)
Pt(S;.D
isthefamilyof all functionspP(S;D
for which the solution function v to(4.lab)
is alsodifferentiable onB,.
Notice thatp
P(S;f)
doesnot imply by itselfthat the solution functionv to(4.lab)
ispositivedefinite with respectto
J. In
fact, pP(S;f)
guaranteesonly existenceof a continuous solution vto(4.12ab)
onany
smallneighborhoodB,
ofJ.
Therefore,aselection ofp
toobeyp P(S;f)
israther apure problem
of solving(4. lab)
than astability problem. Methods forsolving(4. lab)
will notbeconsidered herein.The condition
2)
of Definition means thatp(x)
does notconverge
to zero as x---,0S orIlxll +o,xS. For example, p(x)-O
ifxJ
andt,f)-Cllxll’-l)f2+llxll )
ifxqJ,
andS-Bt-{x’p(x,J)<l}
withJ-{x’llxll <}
obey the condition2). But, p(x)-O
ifxJ
andp(x)-(xll - )(2-Ilxll )
ifxJ,
andS --BI
donotfulfillthe condition2).
Notice thatp
ispositive definite onBI
withrespecttoJ
and differentiable onB
in both cases.Theorem1.
In
orderfor
acompactinvariantsetJ of
thesystem(3.lab)
with theStrong
SmoothnessProperty
tohave the domainD o.f
asymptotic stability andfor
a setN, N
C_R’,
tobethedomainD N D,
it isboth
necessary
andsufficient
that1)
thesetN
isanopen
connected neighborhoodo.f J
andN
C_S,
and2) (a) for
arbitrarilyselectedfunction
pP(S ;f),
theequations(4. lab)
havethe uniquesolution v onN
withthefollowing properties:(i) v ispositive
definite
onN
withrespecttoJ,
(ii) if
theboundary ON of N
isnon-emptythenv(x
+ooasxON,
xN,
or,(b)
for
arbitrarilyselectedpPt(S
;j’)theequations(4.lab)
have theuniquesolution v onN
with the.following properties:(0
visdifferentiable
onN
and positivedefinite
onN
withrespecttoJ,
and(ii) if
theboundary ON of N
isnon-emptythenv(x)
+ooasxON,
xN.
Proof
Necessity.Let
thecompactinvariantsetJ
of thesystem(3. lab)
withtheStrong
SmoothnessProperty
have theasymptotic stabilitydomain
D. Hence,
italsohasDo (Definitions
A-2andA-3 of theAppendix),
which is a connectedopen
neighborhoodofJ.
Evidently,D,
fqS, . Let D C._ S
be firstproved.
If0SthenS
R" andDo
_CS
duetoD
C_R n.
If0S, t thenxo E
0Sandx E (R" ’)
will beanalyzed separately.In
case x0tE 0SthenXo Do
duetotheStrong
SmoothnessProperty. Hence,
0StqDo
and0S t"ID
dueto
D D,,
implied bytheWeak SmoothnessProperty CLemma
A-l, Appendix).In
casex
65(R" -’)
then
x_(t;x)
does notconverge
toJ
dueto theStrong
SmoothnessProperty.
Therefore,x Do
andDfq(R
-S)-9
so thatD CI(R" -S)- 9. From D CIS
"9,D
f3c-
andD f3O(R" -S)-
itresults thatD
C_S. Let N D. Hence, N
C_S
andN
isopenconnectedneighborhoodofJ,
whichproves necessity ofthe condition1).
N -D
implies(Definitions
A-1toA-3)
that10(Xo)-R., fXo
65N.Let
p65P (S ;f), [p 65Pt(S;[)],
be arbitrarilyselected.Hence,
there is a solution v to(3.lab),
which is defined and continuous onB,, [and
differentiable on
B],
respectively,v(x)
65C(-ff,) [v(x)
65C"(-ff ,)] (4.2) Let
"rC]0, +oo[,
"t"t(x0;]’;la’,J),
be such that foranyx0 65N
the condition(4.3)
holds,x_(t;x0)
65B,, Vt
65[x, +o]. (4.3)
Existence of such x isimplied by
N D Do (Definition A-2).
Besides,x_(+oO;Xo) 65, Vx
65N.(4.4)
Afterintegrating
(4.1.a)
andusing(4.1.b)
togetherwith(4.4)
wederive(4.5),
,,[x_(t;x0)] , p[x_(O;Xo)]ao, v(,Xo) R.xV. (4.5)
Invariance of
Do,D Do,N D,
continuity ofmotionsx_ (the
weakSmoothnessProperty),
continuity ofp
onN,
the definitionofx(4.3)
andcompactnessofIt, ;]
forany
65R/ prove
V(t,Xo)
65R/xN (4.6)
+oo,
(4.2), (4.3)
and x(o;xo) x_[o;x;x_ (x;x0)]
65B
foro65Ix, +oo]
and thecondition3)
of Definition 1 yieldp[x(o;x0)]do <+oo,
x065N. (4.7)
Now, (4.5)-(4.7)
givesor, for 0 and x
xo,
v[x_.(t;xo)]J
<+oo,V(t,Xo) 65R+xN, (4.8)
v(x)l
<+oo,Vx
65N.(4.9)
Differentiability of
x_
inXo65N,p
65P(S;./’), [p
65pI(S;f)],
invariance ofND D,,, (4.5)
and(4.8) prove
continuityof v onN,
[differentiability ofvonN],
vCx) C(N) [vCx) C")(N)] (4.10)
respectively. Invarianceof
N,
positivedefinitenessofp
onS
withrespecttoJ,N
C.S,
and(4.5)
implyv(x)
>O, Vx
65(N-J). (4.11)
Now, (4. la), (4.1 0)
and(4.1 1)
verify positivedefiniteness ofv onN
withrespecttoJ [and
itsdifferentiability onN],
respectively. Positivedefiniteness ofp, uniquenessof the motionsx_(t;Xo)
forevery Xo65S,N
C_.S,
invariance ofN
and(4.5) prove
uniquenessof the solutionv to(4. lab).
Thiscompletes
theproof
of necessity ofthe conditions2-a-i)
and2-b-i),
respectively.Let x,
beasequence,x, .
ask +o,.f,65ON, ON
#9,andx,
65N. Let 65]0, +oo[
bearbitrarily selectedso thatB; CN. Let T, T T,(x,;)
65[0, +oo[,
be the first momentsatisfying(4.12),
x(t’,x)B, Vt E[T,+oo[. (4.12)
Such
T
exists due tox N
andN D Do (Definition A-2). Continuity
ofx_(t;Xo)
in(t,Xo) N D, D Do Do
andD
_CS
implyT
+oo ask +o=.Let
m be such a natural number thatx .(N-BOfor
all k -m,m +I,....
Suchm exists becauseNisopen, B CN andxk ON
askLet
cxbe introducedbyct-
min[p(x)’x _(N-BO]. (4.13)
p P(S;f),[p P(S;f)],
guarantees(due
tothe condition2)
of Definition1)
ct
tel0, +oo[. (4.14)
From (4.6)
and(.4.13)
wederive(4.15) by
setting 0andx_(0;x,) x,,
t,
v(x)a foculo+ r,p[x_(o.:t)]do, x (N-J),
k -m,m+(4.15)
lnvarianceofN
-D -Do,
positive definitenessofp
onS
withrespecttoJ (the
condition1)
of Definition1), N
_CS
and(4.16)
implyv(x) T
x(N-J),
k m,m+(4.16)
Thisresult,
T
+ as k + and(4.14)
yieldv(x)
+ooasx ON, x N,
whichproves
necessityof the conditions
2-a-ii)
and2-b-ii),
respectively.Sufficiency.
Let
allconditionsofTheorem be valid. Then,thesetJ
isasymptoticallystable[1, p. 208], [7,
p.204].
Thesystem(3.lab)
has the domainD
ofasymptotic stabilityofJ (Definitions
A-1toA-3).
The condition
1)
impliesN S. Two
possiblecases willbe considered:a)
theboundaryON
ofN
isempty, andb) ON
isnon-empty.a) Let ON -.
ThenN -R"
thatobviously impliesN -D -R"
duetothe conditions 2-a-i and2-b-i).
b) Let ON .
IfOS O#
thenS R"
so thatD C.S.
IfOS ,,
thenc3SfqD due to(ii)
of theStrong
Smoothness
Property.
This fact aswell as that bothD
andS
areneighborhoodsofJ prove D
_CS.In
bothcases
D
C_.S. Let
nowOD ,
andOD
be treatedseparately.
IfOD ,
thenthe definition of v as the solutionto(4.lab), D
_CS
and theproof
of thenecessity partshowthat v is continuousonD
andv(x)
+oasx 0D,xD.
Thesefacts, continuity ofv onN, N C._ S,
thefactthatD
andN
are connectedneighborhoodsofJ
andv(x)
+ooasxON,
xN,
implyN-D (4.17)
Let
nowOD . Hence, D R".
The solution vto(4.lab)
is continuous onD R"
asshown in the necessity part.Hence, v(x)[
<+ooforeveryxER".
Sincev(x)---*
+ooasxON,
x.N,
thenONtqR"and
N -R".
Finally,(4.17)
holds alsoin caseOD ,
whichproves (4.17)
in all casesandcompletes
theproof.
From
thecomputational pointof view theformof the condition"v(x)
+ooasxON, x
U.N"
is notsuitable.It
canbesetinanother formby utilizing
w as usedbyVanelli andVidyasagar[6],
w(x)=
1-exp[-v(x)]. (4.18)
Evidently,thefollowingaretrue:
a)
w isdefined and continuous[and differentiable]
onS
ifandonlyifvisdefined and continuous[and differentiable],
respectively,onS,
b)
positivedefiniteness ofvonS
withrespecttoJ
implies positivedefiniteness of w onS
withrespect toJ,
and viceversa,c) d)
v +ooimpliesw +1 andviceversa,
theequations
(4.lab)
are equivalenttothefollowingsystemdw(x) -[1 w(x)]p(x)
dt
(4.19a)
w(x)-
0,Vx J. (4.19b)
The factslistedabove under
a)
tod)
andTheorem directlyyieldthenextresult:Theorem2.
Let
thefunction
vbereplaced bywand theequations(4.lab) by
theequations(4.19ab)
inDefinition
1.In
orderfor
a compact invariantsetJ of
the system(3.lab)
withtheStrong
SmoothnessProperty
to have the domainD of
asymptotic stability andfor
a setN, N
C_R’,
tobe the domainD N -D,
it isbothnecessary
andsufficient
thattheset
N
isanopenconnectedneighborhoodof J
andN
C_S,
(a)
for
arbitrarilyselectedfunction
pP(S;f),
theequations(4.19ab)
have theuniquesolution w onN
withthefollowing properties:(i) wispositive
definite
onN
withrespecttoJ,
and
(ii)
if
theboundary ONof N
is non-empty thenw(x)
+1 as xON,
xN,
.for
arbitrarilyselectedpPI(S ;f)
theequations(4.19ab)
have theuniquesolution wonN
with thefollowing properties:(i)
wis&fferentiable
onN
andpositivedefinite
onN
withrespecttoJ,
and
(iO if
theboundary ON of N
isnon-emptythenw(x
+1 asxON,
xN.
1)
and
9.)
5.
GENERATION OF A LYAPUNOV FUNCTION AND DETERMINATION OF THE ASYMPTOTIC STABILITY DOMAIN FOR THE SYSTEMS WITH THE WEAK SMOOTHNESS PROPERTY
The class of the systems describedby
(3.lab)
with the WeakSmoothnessProperty
islarger
thanthat with theStrong
SmoothnessProperty. It
is notsurprisingthatthe conditionsof the precedingtheorems slightly changefor thesystemswith the WeakSmoothness propertyasfollows.Theorem3.
In
orderfor
acompactinvariantsetJ of
the system(3.lab)
with theWeakSmoothnessProperty
tohavethe domain
D of
asymptotic stabilityand that a subsetN orS equals D N D,
it isbothnecessary
and
sufficient
that1)
thesetN
isopenconnectedneighborhoodof J,
2) (a) for
arbitrarily selectedfunction p P(R’;f),
theequations(4.lab)
have theuniquesolutionfunction
vonN
withthefollowing properties:(i)
v ispositivedefinite
onN
withrespecttoJ,
and
(ii) if
theboundary ON of N
isnon-emptythenv(x
+asxON,
xN,
or,
(b)
for
arbitrarilyselectedfunction
pP(R’;f),
theequations(4.lab)
have theuniquesolutionfunction
vonN
withthefollowing properties:(i) vis
differentiable
onN
andpositivedefinite
onN
with respecttoJ,
and (ii)if
theboundaryON of N
isnon-emptythenv(x)
+asxON,
xN.
Proof.
Necessity.Let
thesystem(3.lab) possess
theWeakSmoothnessProperty. Let
thesystem(3.lab)
have theasymptotic stabilitydomain
D
and letN-D,
forN
C_S.Let
pP(R";f), [p PI(R";f)],
be arbitrarilyselected.From
thispointon weshouldsimply repeatthecorresponding partof theproof
of necessity of the conditions of Theorem inordertoshownecessityof all conditions of Theorem3.Sufficiency.
Let
the system(3.lab)
have theWeakSmoothnessProperty. Let
the conditionsofTheorem 3hold.Then,the invariantsetJ
isasymptoticallystable.The system(3. lab)
hasthe domainD
of asymptotic stabilityofJ (Definition A-3),
whichequalsDo (Lemma A-l). Letx0 (R" -N).
Continuity ofx_ (t ;x0)
inI0
due to the Weak SmoothnessProperty,
positive definiteness ofp onR"
due topP(R";.f), [p PI(R ;.f)],
negativenessofO(x)
on(R" N)
guaranteed by positivedefinitenessofp onR"
and(4. lab),
andthe condition
2-a-ii), [2-b-ii)],
respectively, implyx_(t;x0) (R" N)
forallI0. Hence, D _C N.
Furthermore,
(4.1a)
and positivedefiniteness ofponR"
imply(see
theproofof the necessitypart of Theorem1) v(x)
+oasxOD,
xD,
whichtogether
withthe condition2-a-i), [2-b-i)],
respectively, impliesOD
fqN, t.
Thisresult,D N
and thefact thatD is aneighborhoodofJ
implyD N
andcomplete
theproof.ThecounterparttoTheorem2inthisframework is thenextresult thatfollowsdirectlyfrom Theorem 3and
(4.18).
Theorem4.
Let
thefunction
vbereplaced by
wand theequations(4.lab) by
theequations(4.19ab)
inDefinition
1.In
orderfor
acompact invariantsetJ of
thesystem(3.lab)
withtheWeakSmoothnessProperty
tohave the domain
D of
asymptotic stabilityand thatasubsetN ors
equalsD N D,
it is bothnecessaryand
sufficient
that1)
thesetN
isopenconnectedneighborhoodof J,
and
2)
(a)for
arbitrarilyselectedfunction
pP(R;f),
theequations(4.19ab)
have theuniquesolution w onN
withthefollowingproperties:(i) w ispositive
definite
onN
withrespecttoJ,
and(iO
if
theboundaryON of N
isnon-empty thenw(x
+ as xON,
xN,
or
(b) for
arbitrarilyselectedfunction
pP(R;f),
theequations(4.19,ab)
have theuniquesolution wonN
withthefollowing properties:(i)
w isdifferentiable
onN
andpositivedefinite
onN
withrespecttoJ,
and(ii)
if
theboundary ON of N
isnon-emptythenw(x
+ asxON,
xN.
6.
GENERATION OF A LYAPUNOV FUNCTION AND ASYMPTOTIC STABILITY
The classicalproblemof the
Lyapunov
stability theory has been theproblem ofthenecessary
and sufficientconditionsforasymptoticstability(without
determination of theasymptotic stabilitydomain).
It
generatedtheproblemof thenecessaryand sufficient conditionsfor an exact, direct and one-shot con- structionof asystemLyapunov
function. The solutiontotheseproblems
resultsdirectly fromtheproof
ofTheorem andTheorem3 in thefollowingform.Theorem5.
In
orderfor
acompactinvariantsetJ of
the system(3.lab)withthe WeakSmoothnessProperty
tobeasymptoticallystableitisboth
necessary
andsufficient
that1) .for
arbitrarilyselectedfunction
p obeyingthe conditions1)
and3) of
(i)ofDefinition
1,theequations(4.lab)
have theunique positivedefinite
solutionfunction
vwithrespecttoJ,
0,
2) for
arbitrarilyselectedfunction
p obeyingthe conditions1)and3) of
(i)and(ii)of Defmition I,
theequations
(4.lab)
have theuniqueeh’fferentiable
positivede.finite
solutionfunction
v withrespecttoJ.
Thistheorem, Theorem andTheorem 3show that the condition
2)
of(i)
of Definition 1isneeded onlyfor the exact determinationoftheasymptotic stabilitydomainD
ofJ.
By
makinguseof(4.18)
the solution can be stated in termsofthe solution w to(4.19ab).
Theorem6.
Let
thefunction
vbereplaced by
wandtheequations(4.lab) by
theequations (4.19ab)
inDefinition
1.In order.for
acompactinvariantsetJ of
thesystem(3.lab)
withtheWeakSmoothnessProperty
tobe
asymptotically
stableit isbothnecessary
andsufficient
that1) for
arbitrarily selectedfunction p
obeyingthe conditions1)
and3) of
(i)of Definition
1,theequations(4.19ab)
have theuniquepositivedefinite
solution w withrespecttoJ,
for
arbitrarilyselectedfunction
p obeying theconditions1)
and3) of
(i)and(ii) of Definition 1,
theequations
(4.19ab)
have theuniquedifferentiable
positivedefinite
solutionfunction
w withrespectto
J.
7. EXAMPLES
Example1.
Let
asimplesecond order nonlinearsystem(3.lab)
have thefollowingspecific
form:dx
2)
d-7-(1-Ilxll (10o- Ilxll )x (7.1)
Thesystemhas theset
S,
of theequilibriumstates,s,- (x:llxll
-0 orIlxll
orIlxll 10}. (7.2)
Theset
J,
J {x: xll 1, (7.3)
isacompactinvariantsetof thesystem.
From (7.1)
and(7.2)
itfollowsthat thesystempossesses
theStrong
SmoothnessProperty
withthesetS
givenbys {x: Ilxll
<10}. (7.4)
Let
the functionp
be selected in the form0
Ilxll -
1,pox)-
(llxil_)llxll Ilxll
1.(7.5)
It
is differentiableonR
andpositivedefinite onR
withrespecttothe setJ (7.3).
Thesolution function v to(4. lab)
forp
definedby(7.5)
is obtained in theformv(x) xll’-
1(7.6)
[98(100_11x11), Ilxll
1.Thefunction v isdefined,continuous and differentiable on the set
S (7.4). Hence, p P(S;f).
Besides,the function vispositivedefinite on
S
withrespecttoJ (7.3)
andv(x)
+ooasxOS,
xS,
where 0s(x: Ilxll 10}.
Since theset
S
isopenconnectedneighborhoodof thesetJ (7.3)
thenall the conditions ofTheorem 1are satisfiedfor thesetN -S (7.4).
Thismeans that thedomainD
ofasymptotic stability of thecompact invariantsetJ (7.3)
ofthesystem(7.1) equals S,
D
-S{x: Ilxll
<10}.
Since the system issimplethisresult can beeasilyverified.
Exalnple2. Letathirdordernonlinearsystem
(3. lab)
be describedby dx2.10’{1 sin[n(2 lO’)-t(xrnx lO)2]}(xrnx- 10)
d-" ncos[n(2 10’)-’ (xrHx 10) 2]
x-./(x),
-?61
10 4
H
-4 10-H r.
-6 2
The matrix
H
ispositivedefinite. The closedinvariant setJ
of thesystemisJ {x :xrHx 10}.
Thesystem
possesses
theStrong
SmoothnessProperty
withthesetS
givenby
S {x :xrnx
<110}. (7.9)
Theset
S (7.9)
isopen
connectedneighborhoodofJ (7.8). Let
the functionp
beaccepted
in the nextform:0 x_J
p(x)=
4(xrHx 10)xrHx
x(R3-,]). (7.10)
Thefunctionpisdefined, continuousand differentiableon
R 3,
andpositivedefinite onR
withrespecttoJ. It
leadstothefollowingsolutionfunctionv totheequations(4.lab),
0 xj
(7.t) v(x)-
-In{I-sin[n(2. 104)-l(xrHx 10)2]},
x(R3-,]).
Thefunctionv
(7.11)
isdefined, continuousand differentiableonS. Hence,
the functionp belongs
toPl(S;f).
Furthermore,the function v(7.11)
isalsopositivedefiniteonS
withrespecttoJ.
Besides,v(x)
+ as xOS {x :xrHx 100}. (7.7)
AllconditionsofTheorem havebeenverified.
Hence,
thesystem(7.7)
has thedomainD
of asymptotic stabilityofJ,
whichequalsN S,
D -S {x:xrHx
<110}.
(7.7a)
(7.8)
8.
CONCLUSION
Nonlinear time-invariantsystemscharacterizedbythe smoothnesspropertiesare considered. The problemsofthenecessaryandsufficientconditionsfor anexactdirect construction of asystem
Lyapunov
function, forasymptotic stabilityofacompactinvariant
setJ
andfortheexactdeterminationofitsasymptotic stabilitydomainaresolvedalgorithmically. Thismeans that the invariantsetJ
isasymptoticallyarable if andonlyif thesolution v to -p(4.1a)
withv(x)
0onJ (4.1b)
ispositivedefinite[and differentiable]
for any p
.P(S;f), [.p PI(S;f)],
respectively. Theequation(4.1a)
is tobesolvedonly
foroneaueharbitrarily
selectedp.
Ifthe solution v ispositivedefinite withrespect
toJ
thenJ
isasymptotically
stable.However,
if the solution vis notpositivedefinitewithrespecttoJ
thenJ
isnotasymptotically
stable.In
the latter case thereis notsensetotrysolving9
-p
withany
other functionp.
Thesestatementsresult from Theorem 5thattogether
with Theorem 6opens
new direction onto theasymptotic
stabilityanalysis.
The completesetsofconditionsforthe exact determinationof the asymptotic
stability
domain ofJ
aregiveninvariousforms of Theorem toTheorem 4.
They
establishessentiallynewapproach
tosolving theLyapunov
stabilityproblems.Ifthe
setJ {0}
and the system(3.lab)
is linearthenTheorem5becomes ageneralization
of the well known criterionforasymptotic stabilityof the zeroequilibriumstateoftime-invariantlinearsystems[5,
p.76].
ACKNOWLEDGEMENT.
Thisresearch wasfinancially supported bythe ScienceFundofSer-
bia,grant number 0401E,throughthe Instituteof Mathematics,Belgrade, Serbia,under thecontract 0401
E,
whiletheauthorwas attheFacultyof MechanicalEngineering,Belgrade,
Serbia,Yugoslavia.APPENDIX A-I. DEFINITIONS OF STABILITY DOMAINS
Definition
A-1.A setJ
of thestatesof thesystem(3.lab)
hasthe domainD,(J) of
stabilityif andonlyiftbrevery
mepsilon ]0, +oo[
there isaneighborhoodD,(e;J)
of thesetJ
such thatx_(t;xo)
belongstothe e-neighborhoodB,(J)
of the setJ
for allE[0,+oo[
provided only that XoD,(e;J)
and thatD,(J) U[D,(e’,J):
e]0, +=o[ ].
Definition
A-2.A
setJ
of thestatesof thesystem(3.lab)
has the domainDo(J) of
attraction if andonly if there is aneighborhoodDo(J)
of thesetJ
such thatlim{p[x(t;x0),J]: +*].
-0 provided onlythatxo
Do(g).
Definition
A-3.A
setJ
of thestatesof thesystem(3.lab)
has the domainD(J) of
asymptotic stabilityif and only if it has both the domainD,(J)
of stability and the domainDo(J)
of attraction andD (J D, (J
f’ID, (J ).
A-II. PROPERTIES OF STABILrrY DOMAINS
Lemma
A-1.If
the system(1)
possessingthe Weak SmoothnessProperty
has the domainD (J of
asymptoticstability
of
asetJ
thenDo(J)
C_D,(J)
andDo(J) D(J).
Proofi Let
thesystem(3.lab) possess
theWeakSmoothnessProperty
andhave the domainD(J).
Then ithas also the domainsD(J)
andD,,(J) (Definition A-3). Letx0 Do(J).
Then,DefinitionA-2and(i-b)
and
(ii)
of the Weak SmoothnessProperty
implymax{p[x_(t’,Xo),J]:te[O,+oo[}-m(x0)
<+oo.Hence,
for
e[m(Xo),+oo[,x(t’,Xo)B,(J),Vte[O,+oo[,
whichproves XotED(e;J),
hence,xoD,(J)
andDo(J)
C_D,(J).
The last result andD(J)- D,(J)tqD,(J) prove Do(J)- D(J).
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J.P.,
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