Volume 2013, Issue 1 310469
Research Article
Open Access

Positive Periodic Solution for Second-Order Singular Semipositone Differential Equations

Xiumei Xing

Corresponding Author

Xiumei Xing

School of Mathematics and Statistics, Yili Normal University, Yining City 835000, China ylsy.edu.cn

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First published: 03 February 2013
Academic Editor: Jifeng Chu

Abstract

We study the existence of a positive periodic solution for second-order singular semipositone differential equation by a nonlinear alternative principle of Leray-Schauder. Truncation plays an important role in the analysis of the uniform positive lower bound for all the solutions of the equation. Recent results in the literature (Chu et al., 2010) are generalized.

1. Introduction

In this paper, we study the existence of positive T-periodic solutions for the following singular semipositone differential equation:
()
where h, aC(R/TZ, R) and the nonlinearity fC((R/TZ)×(0, +) × R, R) satisfies f(t, x, x)≥−M for some M > 0. In particular, the nonlinearity may have a repulsive singularity at x = 0, which means that
()
Electrostatic or gravitational forces are the most important examples of singular interactions.

During the last two decades, the study of the existence of periodic solutions for singular differential equations has attracted the attention of many researchers [14]. Some strong force conditions introduced by Gordon [5] are standard in the related earlier works [6, 7]. Compared with the case of a strong singularity, the study of the existence of periodic solutions under the presence of a weak singularity is more recent [2, 8, 9], but has also attracted many researchers. Some classical tools have been used to study singular differential equations in the literature, including the method of upper and lower solutions [10], degree theory [11], some fixed point theorem in cones for completely continuous operators [12], Schauder’s fixed point theorem [8, 9, 13], and a nonlinear Leray-Schauder alternative principle [2, 3, 14, 15].

However the singular differential equations, in which there is the damping term, that is, the nonlinearity is dependent on the derivative, has not attracted much attention in the literature. Several existence results can be found in [14, 16, 17].

The aim of this paper is to further show that the nonlinear Leray-Schauder alternative principle can be applied to (1) in the semipositone cases, that is, f(t, x, x)≥−M for some M > 0.

The remainder of the paper is organized as follows. In Section 2, we state some known results. In Section 3, the main results of this paper are stated and proved. To illustrate our result, we select the following system:
()
where α > 1,  β > 0,  1 > γ ≥ 0,  μ > 0 is a positive parameter, e(t) is a T-periodic function.

In this paper, let us fix some notations to be used in the following: given φL1[0, T], we write φ≻0 if φ ≥ 0 for almost everywhere t ∈ [0, T] and it is positive in a set of positive measure. The usual Lp-norm is denoted by ∥·∥p. p* and p* the essential supremum and infinum of a given function pL1[0, T], if they exist.

2. Preliminaries

We say that
()
associated to the periodic boundary conditions
()
is nonresonant when its unique solutions is the trival one. When (4)-(5) is nonresonant, as a consequence of Fredholm’s alternative, the nonhomogeneous equation
()
admits a unique T-periodic solution, which can be written as
()
where G(t, s) is the Green’s function of problem (4)-(5). Throughout this paper, we assume that the following standing hypothesis is satisfied.
  • (A)

    The Green function G(t, s), associated with (4)-(5), is positive for all (t, s)∈[0, T]×[0, T].

In other words, the strict antimaximum principle holds for (4)-(5).

Definition 1. We say that (4) admits the antimaximum principle if (6) has a unique T-periodic solution for any l(/T) and the unique T-periodic solution xl(t) > 0 for all t if l≻0.

Under hypothesis (A), we denote
()
Thus B > A > 0 and 0 < ι < 1. We also use w(t) to denote the unique periodic solution of (6) with l(t) = 1 under condition (5), that is, w(t) = (1)(t). In particular, TAw(t) ≤ TB.
With the help of [18, 19], the authors give a sufficient condition to ensure that (4) admits the antimaximum principle in [14]. In order to state this result, let us define the functions
()

Lemma 2 (see [14], Corollary 2.6.)Assume that a≢0 and the following two inequalities are satisfied:

()
where [a(s)] + = max {a(s), 0}. Then the Green’s function G(t, s), associated with (5), is positive for all (t, s)∈[0, T]×[0, T].

Next, recall a well-known nonlinear alternative principle of Leray-Schauder, which can be found in [20] and has been used by Meehan and O’Regan in [4].

Lemma 3. Assume Ω is an open subset of a convex set K in a normed linear space X and p ∈ Ω. Let be a compact and continuous map. Then one of the following two conclusions holds:

  • (I)

    T has at least one fixed point in .

  • (II)

    There exists xΩ and 0 < λ < 1 such that x = λTx + (1 − λ)p.

In applications below, we take with the norm ∥x∥ = max t∈[0,T] | x(t)| and define .

3. Main Results

In this section, we prove a new existence result of (1).

Theorem 4. Suppose that (4) satisfies (A) and

()
Furthermore, assume that there exist three constants M, R0, r > Mw*/ι such that:
  • (H1)

    F(t, x, y) = f(t, x, y) + M ≥ 0 for all (t, x, y)∈[0, T]×(0, r] × R.

  • (H2)

    f(t, x, y) ≥ g0(x) for (t, x, y)∈[0, T]×(0, R0] × R, where the nonincreasing continuous function g0(x) > 0 satisfies and .

  • (H3)

    0 ≤ F(t, x, y)≤(g(x) + h(x))ϱ(|y|),  for  all  (t, x, y)∈[0, T]×(0, r] × R, where g(·) > 0 is nonincreasing in (0, r] and h(·)/g(·) ≥ 0,  ϱ(·) ≥ 0 are nondecreasing in (0, r].

  • (H4)

    ()

  • where

    ()

  • Then (1) has at least one positive periodic solution u(t) with 0 < ∥u + Mw∥≤r.

Proof. For convinence, let us write Z(t) = x(t) − Mw(t), Zn(t) = xn(t) − Mw(t), where w(t) = (1)(t). Let

()
()
First we show that
()
has a solution x satisfying (5), 0 < ∥x∥≤r and Z(t) > 0 for t ∈ [0, T]. If this is true, it is easy to see that Z(t) will be a positive solution of (1)–(5) with 0 < ∥Z + Mw∥≤r.

Choose n0 ∈ {1,2, …} such that 1/n0 < r, and then let N0 = {n0, n0 + 1 + ⋯}.

Consider the family of equations

()
where λ ∈ [0,1],  nN0,  xBr = {x : ∥x∥<r} and Fn(t, x, y) = F(t, max {1/n, x}, y).

A T-periodic solution of (17) is just a fixed of the operator equation

()
where p = 1/n and Tn is a completely continuous operator defined by
()
where we have used the fact
()

We claim that for any T-periodic solution xn(t) of (17) satisfies

()
Note that the solution xn(t) of (17) is also satisfies the following equivalent equation
()
Integrating (22) from 0 to T, we obtain
()

By the periodic boundary conditions, we have x(t0) = 0 for some t0 ∈ [0, T]. Therefore,

()
where we have used the assumption (11) and ∥xn∥<r. Therefore,
()
which implies that (21) holds. In particular, let λFn(t, Z(t), Z(t)) + a(t)/n = 1 in (17), we have
()

Choose n1N0 such that 1/n1R1, and then let N1 = {n1, n1 + 1, …}. The following lemma holds.

Lemma 5. There exists an integer n2 > n1 large enough such that, for all nN2 = {n2, n2 + 1, …},

()

Proof. The lower bound in (27) is established by using the strong force condition of f(t, x, y). By condition (H2), there exists R1 ∈ (0, R0) and a continuous function such that

()
for all (t, x, y)∈[0, T]×(0, R1] × R, where satisfies also the strong force condition like in (H2).

For nN1, let αn = min 0≤tTZn(t),  βn = max 0≤tTZn(t).

If αnR1, due to nN1, (27) holds.

If αn < R1, we claim that, for all nN1,

()
Otherwise, suppose that βnR1 for some nN1. Then it is easy to verify
()
In fact, if 1/nZn(t) ≤ R1, we obtain from (28)
()
and, if Zn(t) ≤ 1/n, we have
()
Integrating (22) (with λ = 1) from 0 to T, we deduce that
()
where estimation (30) and the fact ∥xn∥<r are used. This is a contradiction. Hence (29) holds.

Due to αn < R1, that is, αn = min 0≤tT[xn(t) − Mw(t)] = xn(an) − Mw(an) < R1 for some an ∈ [0, T]. By (29), there exists cn ∈ [0, T] (without loss of generality, we assume an < cn.) such that xn(cn) = Mw(cn) + R1 and xn(t) ≤ Mw(t) + R1 for antcn.

It can be checked that

()
where is defined by (15).

In fact, if t ∈ [an, cn] is such that 1/nZn(t) ≤ R1, we have

()
and, if t ∈ [an, cn] is such that Zn(t) ≤ 1/n, we have
()
So (34) holds.

Using (17) (with λ = 1) for xn(t) and the estimation (34), we have, for t ∈ [an, cn]

()
As , for all t ∈ [an, cn], so Zn(t) is strictly increasing on [an, cn]. We use ξn to denote the inverse function of Zn restricted to [an, cn].

Suppose that (27) does not hold, that is, for some nN1, Zn(t) < 1/n < R1. Then there would exist bn ∈ (an, cn) such that Zn(bn) = 1/n and

()
Multiplying (17) (with λ = 1) by and integrating from bn to cn, we obtain
()

By the facts ∥xn∥ < r,  ,  ∥w∥ ≤ r and the definition of Zn(t), we can obtain , together with ∥xn∥<r, implies that the second term and the third term are bounded. The first term is

()
which is also bounded. As a consequence, there exists a B1 > 0 such that
()
On the other hand, by (H2), we can choose n2N1 large enough such that
()
for all nN2 = {n2, n2 + 1, …}. So (27) holds.

Furthermore, we can prove Zn(t) has a uniform positive lower bound δ.

Lemma 6. There exist a constant δ > 0 such that, for all nN2,

()

Proof. Multiplying (17) (with λ = 1) by and integrating from an to cn, we obtain

()

In the same way as in the proof of (41), one way readily prove that the right-hand side of the above equality is bounded. On the other hand, if nN2, by (H2),

()
if αn → 0+. Thus we know that there exists a constant δ > 0 such that αnδ. Hence (43) holds.

Next, we will prove (17) has periodic solution xn(t).

For ιr > 0, we can choose n3N2 such that 1/n3 < ιr, which together with (H4) imply

()
Let N3 = {n3, n3 + 1, …}. For nN3, consider (17).

Next we claim that any fixed point xn of (18) for any λ ∈ [0,1] must satisfy ∥xn∥≠r. So, by using the Leray-Schauder alternative principle, (17) (with λ = 1) has a periodic solution xn(t). Otherwise, assume that xn is a fixed point xn of (18) for some λ ∈ [0,1] such that ∥xn∥ = r. Note that

()
For nN3, we have
()
By (27) and assumption (H3), for all t ∈ [0, T] and nN3, we have
()
Therefore,
()
This is a contradiction to the choice of n3 and the claim is proved.

The fact ∥xn∥<r and show that is a bounded and equicontinuous family on [0, T]. Now Arzela-Ascoli Theorem guarantees that has a subsequence , converging uniformly on [0, T] to a function xC [0, T]. From the fact ∥xn∥<r and xn(t) > δ, x satisfies δx(t) ≤ r for all t. Moreover, satisfies the integral equation

()
Letting k, we arrive at
()
where the uniform continuity of F(t, x, y) on [0, T]×[δ, r]×[−(r + M)L, (r + M)L] is used. Therefore, x is a positive periodic solution of (16) and Z(t) = x(t) − Mw(t) ≥ δ. Thus we complete the prove of Theorem 4.

Corollary 7. Let the nonlinearity in (1) be

()
where α > 1,  β > 0,  1 > γ ≥ 0,  μ > 0 is a positive parameter, e(t) is a T-periodic function.
  • (i)

    If β + γ < 1, then (1) has at least one positive periodic solution for each μ > 0.

  • (ii)

    If β + γ ≥ 1, then (1) has at least one positive periodic solution for each 0 < μ < μ1, where μ1 is some positive constant.

Proof. We will apply Theorem 4 with M = max 0≤tT | e(t)| and g(x) = xα,  h(x) = μxβ + 2M,  ϱ(y) = 1+|y|γ. Then condition (H1)–(H3) are satisfied and existence condition (H4) becomes

()
So (1) has at least one positive periodic solution for
()
Note that μ1 = if β + γ < 1 and μ1 < if β + γ ≥ 1. We have the desired results.

Acknowledgments

The research of X. Xing is supported by the Fund of the Key Disciplines in the General Colleges and Universities of Xin Jiang Uygur Autonomous Region (Grant no. 2012ZDKK13). It is a pleasure for the author to thank Professor J. Chu for his encouragement and helpful suggestions.

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