STABILITY AND BOUNDEDNESS OF SOLUTIONS FOR A CERTAIN FOURTH-ORDER DELAY DIFFERENTIAL EQUATION∗†
2019-01-09MeilanCaiFanweiMeng
Meilan Cai,Fanwei Meng
(School of Mathematical Sciences,Qufu Normal University,Qufu 273165,Shandong,PR China)
Abstract In this paper,with the help of Lyapunov functional approach,sufficient conditions for the asymptotic stability of zero solution for a certain fourthorder non-linear delay differential equation are given.
Keywords Lyapunov functional approach;asymptotic stability;fourthorder non-linear delay differential equation
1 Introduction
As we know,the stability of zero solution plays an important role in the theory and applications of differential equations.In recent decades,by constructing Lyapunov functions or functionals many results have been obtained on the behaviour of solutions for higher order non-linear ordinary differential equations or higher order non-linear differential equations with delay,see[1-12,14-16].However,it is worth noting that there are only a few papers on the stability of solutions for certain fourth order non-linear differential equations with delay.
In[1],Sinha investigated the asymptotic behaviour of the solutions for a nonlinear differential equations with finite lag
In[2],Tunc considered a fourth-order non-linear delay differential equation
and gave the asymptotic stability of solutions for(1.2).
In[3],the authors studied the fourth-order delay differential equation of the form
and obtained sufficient conditions for the asymptotic stability of solutions.
In this paper,we investigate the same problem for the following fourth-order non-linear delay differential equation
by constructing a new Lyapunov functional,where r is a positive constant,and f4(x)are continuous differential functions and f2(0,0,0)=f3(0)=f4(0)=0,where we assume that the derivativesandexist and are continuous for all x,y,z.The dots indicate differentiation with respect to t.
2 Preliminaries
Before giving the main result of this paper we need the following definitions and stability criteria for the general autonomous delay differential system.We consider
where f:CH→ Rnis a continuous mapping with f(0)=0,CH={ϕ∈C([−r,0],Rn):∥ϕ∥≤ H}and for H1
Definition 2.1[2-4]An element Ψ ∈ CHis in the ω-limit set of ϕ,say,Ω(ϕ),if x(t,0,ϕ)is defined on[0,∞)and there is a sequence{tn}with tn→∞ as n→∞,such that∥xtn(ϕ)−Ψ∥→ 0 as n → ∞,where xtn(ϕ)=x(tn+θ,0,ϕ)for−r≤ θ≤ 0.
Definition 2.2[2-4]A set Q ⊂ CHis an invariant set if for any ϕ ∈ Q,the solution x(t,0,ϕ)for(2.1)is defined on[0,∞),and xt(ϕ)∈ Q for t∈ [0,∞).
Lemma 2.1[2-4]Ifϕ ∈ CHsatisfies that the solutionxt(ϕ)for(2.1)withx0(ϕ)=ϕis defined on[0,∞)and∥xt(ϕ)∥ ≤ H1≤ Hfort∈ [0,∞),thenΩ(ϕ)is a nonempty,compact,invariant set anddist(xt(ϕ),Ω(ϕ))→ 0ast→ ∞.
Lemma 2.2[2-4]LetV:CH→Rbe a continuous functional satisfying a local Lipschitz condition,V(0)=0and that
(i)W1(|ϕ(0)|)≤ V(ϕ)≤ W2(∥ϕ∥)whereW1(r)andW2(r)are wedges;
Then the zero solution for(2.1)is uniformly stable.If we defineZ={ϕ ∈ CH:=0},then the zero solution for(2.1)is asymptotically stable,provided that the largest invariant set inZisQ={0}.
Theorem 2.1[13]LetSandS1be open convex subsets ofX,S0be a closed convex subset ofXwithS0⊂S1⊂S,fbe a compact mapping of S intoX.Supposethat for a positive integerm,fmis well-defined onS1with,whilefm(S1)⊂S0.Thenfhas a fixed point inS0.
Theorem 2.1 is the famous Browder′s fixed point theorem.
3 Main Results
It is obvious that equation(1.4)is equivalent to the following system
First,let
Assume p(t,x,y,z,u,x(t−r),y(t−r))=0,then we get the following theorem.
Theorem 3.1In addition to the fundamental assumptions imposed onf1,f2,f3,andf4,we suppose that there exist positive constantsa,b,c,d, δandε,such that for everyx,y,z,uin,the following conditions are satisfied:
Then the zero solution for system(3.1)is asymptotically stable,provided that
with
Remark 3.1 From conditions(i)and(iii)we can easily obtain
Proof We introduce a Lyapunov function of system(3.1)defined by
where λ and µ are positive constants which will be determined below.
It is easy to see that V(0,0,0,0)=0.We find that the expression of 2V can be rewritten in the following form
where
According to the differential and integral mean value theorem and conditions(ii),(iii),we get
By conditions(i),(iii)and(3.5),we have
From conditions(i)and(iv),we get
By condition(iii),we get
Thus
According to the above discussion,we have
Therefore,it is easy to see that V satisfies condition(i)of Lemma 2.2.By the identity
for direct calculation,we get the total derivative of(3.3)with respect to t along the solutions of system(3.1)as follows
By conditions(ii)and(iv),we get
By conditions(iii)and(iv),we obtain
From conditions(i),(ii),(iv)and(3.2),we have
By condition(v),we get
From condition(vi),we have
Based on the above discussion,we can easily get
Now,we let
and
which is contained in equation(3.11).
From condition(v),we get the inequalities
and
then it follows that
Then we obtain
Letting λ=d(m+n+1)/2>0 andµ=ab(m+n+1)/2>0,there is
Thus,if
we have
The proof of Theorem 3.1 is now complete.
Let p(t,x,y,z,u,x(t− r),y(t− r))≠0,then we get the following theorems.
Theorem 3.2We suppose that all the conditions of Theorem3.1and
hold,whereq ∈ L1(0,∞)withL1(0,∞)being the space of Lebesgue integrable functions satisfies∫|q(s)|ds≤Q0<∞,andQ0is a positive constant.Then there exists a finite positive constantKsuch that all solutionsx(t)for(1.4)defined by the initial function
satisfy
for allt≥ t0,whereψ ∈ C3([t0−r,t0],R),provided that
with
Proof From(3.9)we have
where
According to(3.21),we obtain
where D2=max{m,n,1}.
Making use of inequalities|y|<1+y2,|z|<1+z2and|u|<1+u2,it is obvious that
By(3.22),we get
Therefore,
Now,integrating inequality(3.26)from 0 to t,using the condition q∈ L1(0,∞)and Gronwall-Reid-Bellman inequality,we have
Obviously,the right-hand side is a finite constant,denoted as K1.
By inequalities(3.22)and(3.27),we have
where K2=.Therefore,we can deduce that
for all t≥t0.
The proof of Theorem 3.2 is completed.
Theorem 3.3In addition to the conditions of Theorem3.1,we also assume that there exist continuous functionsθ1(t)andθ2(t),such thatp(t,x,y,z,u,v,w)satisfies
uniformly int≥ 0,whereθ1(t)andθ2(t)satisfy
andis sufficiently small.Then the solutions of system(3.1)are uniformly ultimately bounded.
Proof Since p(t,x,y,z,u,v,w)satisfies(3.29),by(3.21)and Schwarz′s inequality we have
By(3.30),we have
and
Then
where
By Theorem 3.1 and Theorem 8.10 in Yoshizawa[17],solutions of(3.1)are uniformly ultimately bounded.
The proof of Theorem 3.3 is completed.
Theorem 3.4We assume that all the conditions of Theorem3.3are satisfied,and thatp(t,x,y,z,u,v,w)satisfies
then there exists at least oneω-periodic solution for(3.1).
Proof By the Theorem 3.3,we obtain that all solutions for(3.1)are uniformly ultimately bounded for bound M(M≥K).
Consider the Poincaré map
Since the solution of(3.1)are uniformly bounded,there exists a q(M)>0,such that if t0∈ I=[0,∞)and(x0,y0,z0,u0)∈,where
Then
Similarly,there exist two constant r and r∗such that if t0∈ I and(x0,y0,z0,u0)∈with Sq={(x,y,z,u):|x| and if t0∈I,(x0,y0,z0,u0)∈with Sr={(x,y,z,u):|x| Let S=Sr,then T(S)⊂∗and T is continuous.Thus,T is a compact mapping. Since solutions of(3.1)are uniform-ultimately bounded for bound M,there exists a τ>0,such that if t≥ τ and(x0,y0,z0,u0)∈ Sq,then Then there exists a positive integer m such that for(x0,y0,z0,u0)∈Sq. According to Theorem 2.1,the Poincaré map T has a fixed point(x0,y0,z0,u0)in,that is, The proof of Theorem 3.4 is completed. Remark 3.2 Theorems 3.1 and 3.2 are different with Theorems 3.1 and 3.3 in[14],respectively.Furthermore,the results of Theorems 3.3 and 3.4 only be studied in this paper.
杂志排行
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