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In this article, we study a class of Li´enard equations x00(t) +f(x(t))x0(t) +g1(x(t)) +g2(x(t−τ(t)) =e(t)

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ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu

UNIFORM BOUNDEDNESS OF SOLUTIONS FOR A CLASS OF LI ´ENARD EQUATIONS

GUO-RONG YE, HUI-SHENG DING, XI-LANG WU

Abstract. In this article, we study a class of Li´enard equations x00(t) +f(x(t))x0(t) +g1(x(t)) +g2(x(tτ(t)) =e(t).

Under some suitable conditions, we ensure that all solutions of the above Li´enard equations are uniformly bounded. Our assumptions are less restrictive than those in [9]; thus we extend some previous results.

1. Introduction

As it is we all know, Li´enard equations appears in a number of physical models and is important in describing fluid mechanical and nonlinear elastic mechanical phenomena. Thus, there has been great interest for many mathematicians to study the dynamical behavior of all kinds of Li´enard equations (cf. [1, 3, 6, 8, 9, 10, 11, 12, 4, 5] and references therein). Especially, several authors have contributed to the study on boundedness of solutions to Li´enard equations (cf. [6, 8, 10, 9, 12] and references therein). For example, in 1998, the authors in [6] discussed the bounded solutions of the Li´enard equation

x00(t) +f(x)x0+g(x) =e(t).

Recently, the authors in [10] studied the boundedness of solutions to the following Li´enard equation with a deviating argument:

x00(t) +f(x(t))x0(t) +g1(x(t)) +g2(x(t−τ(t))) =e(t), (1.1) wheref,g1andg2are continuous functions onR,τ(t)≥0 is a bounded continuous function onR, ande(t) is a bounded continuous function on R+= [0,+∞).

The authors in [10] established a theorem which ensure that all solutions of (1.1) are uniformly bounded, under the following two assumptions:

(C1) There exists a constantd > 1 such that d|u| ≤ sgn(u)ϕ(u) for all u∈R, where

ϕ(u) = Z u

0

[f(x)−1]dx.

(C2) There exist nonnegative constantsL1, L2, q1, q2such thatL1+L2<1 and

|g1(u)−ϕ(u)| ≤L1|u|+q1, |g2(u)| ≤L2|u|+q2, ∀u∈R.

2000Mathematics Subject Classification. 34K25.

Key words and phrases. Li´enard equation; boundedness of solutions.

c

2009 Texas State University - San Marcos.

Submitted May 15, 2009. Published August 11, 2009.

1

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In this article, we will make further study on this problem. As one will see, under weaker assumptions than (C1) and (C2), we also get the same conclusion to [10]. Next, let us recall some notations and basic results.

Throughout this paper, we denote ϕ(x) =

Z x 0

[f(u)−1]du, y=dx

dt +ϕ(x).

Then (1.1) is transformed into the system dx(t)

dt =−ϕ(x(t)) +y(t), dy(t)

dt =−y(t)−[g1(x(t))−ϕ(x(t))]−g2(x(t−τ(t)) +e(t).

(1.2)

Leth= supt∈Rτ(t)≥0. C([−h,0],R) denotes the space of continuous functions φ: [−h,0]→R with the supremum norm k · k. It is well known (cf. [2, 7]) that for any given continuous initial functionφ∈C([−h,0],R) and a numbery0, there exists a solution of (1.2) on an interval [0, T) satisfying the initial conditions and (1.2) on [0, T). If the solution remains bounded, thenT = +∞. We denote such a solution byx(t) =x(t, φ, y0),y(t) =y(t, φ, y0).

Definition 1.1 ([10]). Solutions of (1.2) are called uniformly bounded if for each B1>0 there is aB2>0 such that (φ, y0)∈C([−h,0],R)×Randkφk+|y0| ≤B1

implies that|x(t, φ, y0)|+|y(t, φ, y0)| ≤B2 for allt∈R+. 2. Main results For our convenience, we list the following assumptions:

(A1) |u|<sgn(u)ϕ(u) for allu∈R.

(A2) There exist two nondecreasing functions G,Φ defined onR+ such that

|g1(u)−ϕ(u)| ≤Φ(|u|), |g2(u)| ≤G(|u|), ∀u∈R, lim sup

x→+∞

[Φ(x) +G(x)−x+e]<0, e= sup

t∈R+

|e(t)|.

Theorem 2.1. Suppose that(A1), (A2)hold. Then solutions of (1.2)are uniformly bounded.

Proof. Letx(t) = x(t, φ, y0), y(t) = y(t, φ, y0) be a solution of (1.2). Calculating the upper right derivatives of|x(s)| and|y(s)|, in view of (A1) and (A2), we have

D+(|x(s)|)|s=t= sgn(x(t)){−ϕ(x(t)) +y(t)}

<−|x(t)|+|y(t)|,

D+(|y(s)|)|s=t= sgn(y(t)){−y(t)−[g1(x(t))−ϕ(x(t))]−g2(x(t−τ(t)) +e(t)}

≤ −|y(t)|+ Φ(|x(t)|) +G(|x(t−τ(t))|) +e.

Let

M(t) = max

−h≤s≤t{max{|x(s)|,|y(s)|}}, t≥0.

By (A2), there is a constantM >0 such that

Φ(x) +G(x)−x+e <0, x≥M. (2.1) For any givent0≥0, we consider five cases.

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Case (i): M(t0) >max{|x(t0)|,|y(t0)|}. It follows from the continuity of x(t) andy(t) that there existsδ1>0 such that

max{|x(t)|,|y(t)|}< M(t0), ∀t∈(t0, t01).

Thus, one can concludeM(t) =M(t0), for allt∈(t0, t01).

Case (ii): M(t0) = max{|x(t0)|,|y(t0)|} < M. Also, by the continuity ofx(t) andy(t), there exists δ2>0 such that

max{|x(t)|,|y(t)|}< M, ∀t∈(t0, t02).

Therefore,M(t)< M, for allt∈(t0, t02).

Case (iii): M(t0) = max{|x(t0)|,|y(t0)|}= |x(t0)| ≥ M, and |x(t0)| > |y(t0)|.

Since

D+(|x(s)|)|s=t0 <−|x(t0)|+|y(t0)|<0, there exists δ3>0 such that

|x(t)|<|x(t0)|=M(t0) ∀t∈(t0, t03).

On the other hand, by the continuity ofy(t), without loss, one can assume that

|y(t)|<|x(t0)|=M(t0), ∀t∈(t0, t03).

So

max{|x(t)|,|y(t)|}< M(t0), ∀t∈(t0, t03), which impliesM(t) =M(t0), for allt∈(t0, t03).

Case (iv): M(t0) = max{|x(t0)|,|y(t0)|}= |y(t0)| ≥ M, and |x(t0)| < |y(t0)|.

By (2.1), we have

D+(|y(s)|)|s=t0 ≤ −|y(t0)|+ Φ(|x(t0)|) +G(|x(t0−τ(t0))|) +e

≤ −M(t0) + Φ(M(t0)) +G(M(t0)) +e <0, which yields that there existsδ4>0 such that

|y(t)|<|y(t0)|=M(t0), ∀t∈(t0, t04).

On the other hand, without loss of generality, one can assume that

|x(t)|<|y(t0)|=M(t0), ∀t∈(t0, t04).

So one can conclude

max{|x(t)|,|y(t)|}< M(t0), ∀t∈(t0, t04).

ThusM(t) =M(t0) for allt∈(t0, t04).

Case (v): M(t0) = max{|x(t0)|,|y(t0)|}=|x(t0)|=|y(t0)| ≥M. We have D+(|x(s)|)|s=t0 <−|x(t0)|+|y(t0)|= 0.

Also, similar to the proof of Case (iv), one can show that D+(|y(s)|)|s=t0 <0.

Thus, there existsδ5>0 such that

|x(t)|<|x(t0)|=M(t0), |y(t)|<|y(t0)|=M(t0) ∀t∈(t0, t05).

Therefore,M(t) =M(t0) for allt∈(t0, t05). In summary, for eacht0≥0, there existsδ >0 such that

M(t)≤max{M(t0), M}, ∀t∈(t0, t0+δ).

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Let

α=









inf{t≥0 :M(t)>max{M(0), M}}

if{t≥0 :M(t)>max{M(0), M}} 6=∅, +∞

if{t≥0 :M(t)>max{M(0), M}}=∅.

We claim thatα= +∞. Ifα <+∞, then

M(t)≤max{M(0), M}, ∀t∈[0, α]. (2.2) It follows from the above proof that there is a constantδ0 >0 such that

M(t)≤max{M(α), M}, ∀t∈(α, α+δ0). (2.3) Combing (2.2) and (2.3), we have

M(t)≤max{M(0), M}, ∀t∈[0, α+δ0),

which yieldsα≥α+δ0. This is a contradiction. Thus,α= +∞, which implies M(t)≤max{M(0), M}, ∀t≥0.

Then, we have

|x(t)| ≤max{M(0), M}, |y(t)| ≤max{M(0), M}, ∀t≥0.

Therefore, solutions of (1.2) are uniformly bounded.

Remark 2.2. One can easily conclude (A1) and (A2) from the assumptions (C1) and (C2). So Theorem 2.1 is a generalization of [10, Theorem 3.1]. In addition, our assumptions are weaker than (C1) and (C2) in essence (see Remark 2.4).

Next, we give an example to illustrate our results.

Example 2.3. Consider the following Li´enard equation:

x00(t) +f(x(t))x0(t) +g1(x(t)) +g2(x(t−τ(t)) =e(t), (2.4) where

f(x) = e−x−xe−x

2 + 2, g1(x) = xe−x+ 3x+x1/3

2 ,

g2(x) =x1/3, τ(t) = cos2t, e(t) = sint.

Then

ϕ(x) = Z x

0

[f(u)−1]du=1

2xe−x+x, and

sgn(x)ϕ(x) = 1

2e−x+ 1

|x|>|x|, ∀x∈R. So (A1) holds. In addition, let

Φ(x) = x+x1/3

2 , G(x) =x1/3. Then

|g1(u)−ϕ(u)|=

u+u1/3 2

≤Φ(|u|), |g2(u)|=G(|u|), ∀u∈R,

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and

lim sup

x→+∞

[Φ(x) +G(x)−x+e] = lim sup

x→+∞

x+x1/3

2 +x1/3−x+ 1

<0, e= sup

t∈R+

|e(t)|= 1.

So (A2) holds. Then Theorem 2.1 shows that solutions of (2.4) are uniformly bounded.

Remark 2.4. In the above example, there is no a constantd >1 such that sgn(x)ϕ(x)≥d|x|, ∀x∈R.

So (C1) does not hold. Thus, [10, Theorem 3.1] can not be applied.

Acknowledgments. Hui-Sheng Ding acknowledges support from the NSF of China (10826066), the NSF of Jiangxi Province of China (2008GQS0057), the Youth Foun- dation of Jiangxi Provincial Education Department (GJJ09456), and the Youth Foundation of Jiangxi Normal University. Guo-Rong Ye and Xi-Lang Wu acknowl- edge support from the Graduate Innovation Foundation of Jiangxi Normal Univer- sity (JXSD-Y-09045).

References

[1] C. Bereanu; Multiple periodic solutions of some Li´enard equations with p-Laplacian, Bull.

Belg. Math. Soc. Simon Stevin 15 (2008), 277–285.

[2] T. A. Burton; Stability and Periodic Solutions of Ordinary and Functional Differential Equa- tions, Academic Press, Orland, FL, 1985.

[3] N. P. C´ac; Periodic solutions of a Li´enard equation with forcing term, Nonlinear Anal. 43 (2001), 403–415.

[4] P. Cieutat; On the structure of the set of bounded solutions on an almost periodic Li´enard equation, Nonlinear Anal. 58 (2004), 885–898.

[5] P. Cieutat; Almost periodic solutions of forced vectorial Li´enard equations, J. Differential Equations 209 (2005), 302–328.

[6] A. Fonda, F. Zanolin; Bounded solutions of nonlinear second order ordinary differential equa- tions, Discrete and Continuous Dynamical Systems, 4 (1998), 91–98.

[7] J. K. Hale; Theory of Functional Differential Equations, Springer-Verlag, New York, 1977.

[8] L. Huang, Y. Cheng, J. Wu; Boundedness of solutions for a class of nonlinear planar systems, Tohoku Math. J. 54 (2002), 393–419.

[9] B. Liu, L. Huang; Boundedness for a class of retarded Li´enard equation, J. Math. Anal. Appl.

286 (2003), 422–434.

[10] B. Liu, L. Huang; Boundedness of solutions for a class of Li´enard equations with a deviating argument, Appl. Math. Lett. 21 (2008), 109–112.

[11] B. Toni; Almost and pseudo-almost limit cycles for some forced Li´enard systems, Nonlinear Anal., in press.

[12] G. Villari; On the qualitative behavior of solutions of the Li´enard equation, J. Differential Equations 67 (1987) 267–277.

College of Mathematics and Information Science, Jiangxi Normal University, Nan- chang, Jiangxi 330022, China

E-mail address, G.-R. Ye: [email protected] E-mail address, H.-S. Ding: [email protected] E-mail address, X.-L. Wu: [email protected]

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