On the existence of periodic solutions for a class of generalized forced Liénard equations
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AppliedMathematicsLetters20(2007)
248–254
www.elsevier.com/locate/aml
Ontheexistenceofperiodicsolutionsforaclassofgeneralized
forcedLi´enardequations✩
M.R.Pournakia,∗,A.Razanib,a
aSchoolofMathematics,InstituteforStudiesinTheoreticalPhysicsandMathematics,P.O.Box19395-5746,Tehran,Iran
bDepartmentofMathematics,FacultyofScience,ImamKhomeiniInternationalUniversity,P.O.Box34194-288,Qazvin,Iran
Received14July2005;receivedinrevisedform28May2006;accepted2June2006
Abstract
Inthisworkthesecond-ordergeneralizedforcedLi´enardequationx+
f(x)+k(x)x
x+g(x)=p(t)isconsideredanda
newconditionforguaranteeingtheexistenceofatleastoneperiodicsolutionforthisequationisgiven.
c2006ElsevierLtd.Allrightsreserved.
Keywords:Nonlinearboundaryvalueproblem;Li´enardequation;Periodicsolution;Banachspace;Schauder’sFixedPointTheorem
1.Introduction
Inthisworkweinvestigatetheexistenceofperiodicsolutionsforaclassofsecond-ordergeneralizedforcedLi´enard
equations
x+
f(x)+k(x)x
x+g(x)=p(t),(1.1)
wheref,k,andgarerealfunctionsonRandpisaT-periodicrealfunctionon[0,T],T>0.Generalizedforced
Li´enardequationsappearinanumberofphysicalmodelsandanimportantquestioniswhethertheseequationscan
supportperiodicsolutions.Thisquestionhasbeenstudiedextensivelybyanumberofauthors;seeforexample[1–9].
Inparticular,therearesomeexistenceandmultiplicityresultsforsuchequationswithnonconstantforcedterms;see
forexample[10–19].Inthisdirection,wewillobtainanewconditiontoguaranteetheexistenceofatleastoneperiodic
solutionfor(1.1)withanonconstantforcedterm.Themainpurposeofthisworkistoprovethefollowingresult:
MainTheorem.Supposef,k,andgarerealfunctionsonRwhicharelocallyLipschitzandpisanonconstant,
continuous,T-periodicrealfunctionon[0,T],T>0.Alsosupposeallsolutionsoftheinitialvalueproblem(1.1)
canbeextendedto[0,T].Ifthereexistrealnumbersa1anda2forwhichg(a1)≤p(t)≤g(a
2)holdsforeach
0≤t≤T,thenEq.(1.1)hasatleastoneperiodicsolution.
✩ThisresearchwasinpartsupportedbyagrantfromIPM.
∗Correspondingauthor.
E-mailaddresses:pournaki@ipm.ir(M.R.Pournaki),razani@ikiu.ac.ir(A.Razani).
0893-9659/$-seefrontmatterc2006ElsevierLtd.Allrightsreserved.
doi:10.1016/j.aml.2006.06.004M.R.Pournaki,A.Razani/AppliedMathematicsLetters20(2007)248–254249
Therestoftheworkisorganizedasfollows.InSection2,weprovethat(1.1)hasauniquesolutionsatisfying
certainconditionsbyapplyingSchauder’sFixedPointTheorem.InSection3,theexistenceofatleastoneperiodic
solutionfor(1.1)whenghasthepropertymentionedintheMainTheoremisproved.
2.Anexistenceanduniquenesstyperesult
WestartthissectionbyrecallingafamousfixedpointtheoremwhichwasoriginallyduetoSchauder:LetXbea
BanachspaceandΩbeaclosed,bounded,andconvexsubspaceofX.IfS:Ω→Ωisacompactoperator,thenS
hasatleastonefixedpointonΩ.
WenowstateandprovethefollowingexistenceanduniquenesstyperesultwhichisakeytoolforprovingtheMain
Theorem.
Proposition2.1.Leta1
2andB>0berealnumbersandconsiderA=max{2|a1|,2|a
2|}.Supposef,k,and
garerealfunctionsonRwhicharelocallyLipschitzandatleastoneofthef,k,orgisnonconstanton|x|≤A;
andpisacontinuousT-periodicrealfunctionon[0,T],T>0.AlsosupposeM0isthemaximumvalueof|p|on
[0,T];M
1,M
2,M
3arethemaximumvaluesof|f|,|k|,|g|on|x|≤A;andM
1,M
2,M
3aretheLipschitzconstants
off,k,gon|x|≤A,respectively.Consider
M=2
M
2B2+(2M
2+M
1)B+M
3+M
1,
N=1
M2B2+M
1B+M3+M
0,and0
0
T,2√
AN,2BN,2√
M+1−2
.
Thenforeacha1≤b≤a
2,Eq.(1.1)hasauniquesolutionx(t),satisfying
x(0)=x(T0)=b,(2.1)
forwhich|x(t)|≤Aand|x(t)|≤Bholdforeach0≤t≤T
0.
Proof.Considertheequationx=0withboundaryconditionx(0)=x(T
0)=b.TheexistenceofaGreen’sfunction
foratypicaltwo-endpointproblemwassuggestedbyasimplephysicalexamplein[20]andisasfollows:
G(t,s)=
s(t−T0)/T
0:if0≤s≤t≤T
0,
t(s−T0)/T
0:if0≤t≤s≤T
0.
Ifwenowconsidertheintegralequation
x(t)=b+
T0
0G(t,s)
f(x(s))+k(x(s))x(s)
x(s)+g(x(s))−p(s)
ds,(2.2)
thenitiseasytoseethatthesolutionsof(2.2)areexactlythesolutionsof(1.1)satisfying(2.1).Hence,toprovethe
proposition,itisenoughtoshowthat(2.2)hasauniquesolutionx(t)satisfying|x(t)|≤Aand|x(t)|≤Bforeach
0≤t≤T0.Inordertodoso,supposeX=C1([0,T
0],R),andforφ∈Xdefine
φ=max
0≤t≤T0|φ(t)|+max
0≤t≤T0|φ(t)|.
ItisclearthatXisaBanachspace.Now,consider
Ω=
φ∈X:|φ(t)|≤Aand|φ(t)|≤Bholdforeach0≤t≤T
0
,
whichisobviouslyaclosed,bounded,andconvexsubspaceofX.DefinetheoperatorS:Ω→Xbymappingφto
S(φ),whereS(φ)isdefinedby
S(φ)(t)=b+
T0
0G(t,s)
f(φ(s))+k(φ(s))φ(s)
φ(s)+g(φ(s))−p(s)
ds.