# Asymptotic problems for fourth-order nonlinear differential equations

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## Abstract

We study vanishing at infinity solutions of a fourth-order nonlinear differential equation. We state sufficient and/or necessary conditions for the existence of the positive solution on the half-line $[0,\mathrm{\infty})$ which is vanishing at infinity and sufficient conditions ensuring that all eventually positive solutions are vanishing at infinity. We also discuss an oscillation problem.

### Keywords

Quasilinear Equation Homoclinics Solution Nonoscillatory Solution Oscillation Problem Asymptotic Boundary Condition## Dedication

Dedicated to Jean Mawhin on occasion of his seventieth birthday.

## 1 Introduction

where $\lambda \ge 1$, $q\in {C}^{3}({\mathbb{R}}_{+})$, $q(t)>0$ for large *t*, $r\in C({\mathbb{R}}_{+})$ such that $r(t)\ne 0$ for large *t* and ${\mathbb{R}}_{+}=[0,\mathrm{\infty})$.

By a solution of (1) we mean a function $x\in {C}^{4}[{T}_{x},\mathrm{\infty})$, ${T}_{x}\ge 0$, which satisfies (1) on $[{T}_{x},\mathrm{\infty})$. A solution is said to be *nonoscillatory* if $x(t)\ne 0$ for large *t*; otherwise, it is said to be *oscillatory*. Observe that if $\lambda \ge 1$, according to [[1], Theorem 11.5], all nontrivial solutions of (1) satisfy $sup\{|x(t)|:t\ge T\}>0$ for $T\ge {T}_{x}$, on the contrary to the case $\lambda <1$, when nontrivial solutions satisfying $x(t)\equiv 0$ for large *t* may exist.

Fourth-order differential equations have been investigated in detail during the last years. The periodic boundary value problem for the superlinear equation ${x}^{(4)}=g(x)+e(t)$ has been studied in [2]. In [3], the fourth-order linear eigenvalue problem, together with the nonlinear boundary value problem ${x}^{(4)}-f(t,x)=0$, has been investigated. Oscillatory properties of solutions for self-adjoint linear differential equations can be found in [4]. Equation (1) with $q(t)\equiv 0$ can be viewed as a prototype of even-order two-term differential equations, which are the main object of monographs [1, 5, 6].

Equation (1′) with $q(t)\equiv 1$ for $t\in {\mathbb{R}}_{+}$ is a special case of higher-order differential equations investigated in [7]. Equation (1′) with *q* near to a nonzero constant as $t\to \mathrm{\infty}$ has been considered in [8] as a perturbation of the linear equation ${y}^{(4)}(t)+q(t){y}^{\u2033}(t)=0$, and the existence of oscillatory solutions of (1′) has been proved. In [9], necessary and sufficient conditions for the existence of asymptotically linear solutions of (1′) have been given.

where $k\in \mathbb{R}$, $f(u)u>0$ for $u\ne 0$, and $f\in {Lip}_{\mathrm{loc}}(\mathbb{R})$ has been investigated and applications to the biharmonic PDE’s can be found there. In particular, the so called *homoclinics solutions*, which are defined as nontrivial solutions *x* such that ${lim}_{t\to \pm \mathrm{\infty}}x(t)=0$, are studied.

A solution *x* of (1) satisfying (3) is said to be *vanishing at infinity*.

*Kneser problem*for (1). The Kneser problem is a problem concerning the existence of solutions of (1) subject to the boundary conditions on the half-line $[0,\mathrm{\infty})$

We establish necessary and/or sufficient conditions for the solvability of the boundary value problem (1), (3), (4). In the light of these results, as the second problem, we study when all eventually positive solutions *x* of (1) are vanishing at infinity assuming that $\lambda >1$ and (2) is oscillatory. As a consequence, we give a bound for the set of all nonoscillatory solutions. Finally, we discuss when problem (1), (3) is not solvable and solutions to (1) are oscillatory.

*h*is a positive solution of (2). According to [11], a solution

*h*of (2) is said to be a

*principal solution*if ${\int}^{\mathrm{\infty}}{h}^{-2}(t)\phantom{\rule{0.2em}{0ex}}dt=\mathrm{\infty}$, and such a solution is determined uniquely up to a multiple constant. Since $q(t)>0$, every eventually positive solution of (2) is nondecreasing for large

*t*. Hence there exists a principal solution

*h*of (2) such that $h(t)>0$ for $t\ge a\ge 0$ and

Therefore, we can use the known results [12, 13] stated for systems of differential equations or in [14] for fourth order differential equations.

If (2) is oscillatory, then our approach is based on the choice of a suitable transformation. The main idea is based on a transformation of (1) to the fourth-order quasilinear equation and the use of the estimates for positive solutions of such an equation on a compact interval stated in [15]. This, together with an energy function associated with (1), enables us to state an oscillation theorem. In the final section, some extensions of our results to (1′) are given.

## 2 The Kneser problem

In this section we present necessary and/or sufficient conditions for solvability of boundary value problem (1), (3), (4).

### 2.1 Case $r(t)<0$

**Proposition 1** *Let* $\lambda \ge 1$, (2) *be disconjugate on* $[0,\mathrm{\infty})$, *and* $r(t)<0$ *for* $t\in {\mathbb{R}}_{+}$. *Then boundary value problem* (1), (4) *is solvable for any* $c>0$.

where we restrict to the case that $f=({f}_{1},{f}_{2},{f}_{3},{f}_{4}):{\mathbb{R}}_{+}\times {\mathbb{R}}^{4}\to {\mathbb{R}}^{4}$ are continuous functions, $n=4$, $m=1$, $l=2$, $a=1$ and $r=c$. Then this result reads as follows.

**Theorem A** ([12])

*Let there exist*$c>0$

*such that*

*for*$t\in {\mathbb{R}}_{+}$, ${y}_{1}\in [0,c)$, ${y}_{i}\in {\mathbb{R}}_{+}$ ($i=2,3,4$).

*Suppose*

*for*$t\in [0,1]$, ${y}_{1}\in [0,c]$, ${y}_{i}\in {\mathbb{R}}_{+}$ ($i=2,3,4$),

*where functions*${\phi}_{i}:[0,1]\times {\mathbb{R}}_{+}\to {\mathbb{R}}_{+}$ ($i=1,2,3$)

*are continuous and nondecreasing in the second argument such that*

*is a continuous function and*$\omega :{\mathbb{R}}_{+}\to (0,\mathrm{\infty})$

*is a continuous nondecreasing function such that*

*Then*,

*for any*${x}_{0}\in [0,c]$,

*system*(7)

*has a solution satisfying*

*Proof of Proposition 1*Assume $r(t)<0$ for $t\in {\mathbb{R}}_{+}$. Since (2) is disconjugate, it has a positive solution

*h*on ${\mathbb{R}}_{+}$, and (1) can be written as (5) where $h(t)r(t)<0$ on ${\mathbb{R}}_{+}$. Let

*x*be a solution of (5) and denote

Since $\lambda \ge 1$, system (10) has no solutions such that ${y}_{i}\equiv 0$ for some $i=1,2,3,4$ and large *t*; see [16] or [[17], Lemma 2, Theorem 2]. Thus, for any $c>0$, equation (1) has a solution *x* such that $x(0)=c$, $x(t)={y}_{1}(t)>0$, ${x}^{\prime}(t)=-{y}_{2}(t)<0$ and ${x}^{\u2033}(t)=h(t){y}_{3}(t)>0$ for $t\ge 0$. □

Now we state conditions for the existence of a solution for problem (1), (3), (4).

**Theorem 1**

*Let*$\lambda \ge 1$, $r(t)<0$

*and*

*on*${\mathbb{R}}_{+}$.

*If*

*then problem* (1), (3), (4) *is solvable for any* $c>0$.

*In addition*,

*if*

*then the condition*

*is necessary and sufficient for the solvability of problem* (1), (3), (4).

For the proof, the following lemma will be needed.

**Lemma 1**

*Consider system*(10)

*on*$[a,\mathrm{\infty})$ ($a\ge 0$),

*where*$h(t)>0$

*for*$t\ge a$

*and*

*h*

*is a principal solution of*(2).

*Let*$y=({y}_{1},{y}_{2},{y}_{3},{y}_{4})$

*be a solution of*(10)

*such that*${y}_{i}(t)\ge 0$

*and*${y}_{i}^{\mathrm{\prime}}(t)\le 0$

*for*$i=1,2,3,4$,

*and*$t\ge a$.

*Then*${lim}_{t\to \mathrm{\infty}}{y}_{i}(t)=0$

*for*$i=2,3,4$,

*and if*

*then* ${lim}_{t\to \mathrm{\infty}}{y}_{1}(t)=0$, *too*. *Vice versa*, *if* $\lambda \ge 1$ *and* ${lim}_{t\to \mathrm{\infty}}{y}_{1}(t)=0$, *then* (15) *holds*.

*Proof*In view of the monotonicity of ${y}_{i}$, there exist ${lim}_{t\to \mathrm{\infty}}{y}_{i}(t)={y}_{i}(\mathrm{\infty})\ge 0$, $i=1,2,3,4$. Since

*h*is the principal solution, (6) holds, and integrating the first three equations in (10) from

*a*to

*t*, we get ${y}_{i}(\mathrm{\infty})=0$ for $i=2,3,4$. Now integrating (10) from

*t*to ∞, we have

Letting $t\to \mathrm{\infty}$ and using the change of the order of integration, we get a contradiction with the boundedness of ${y}_{1}$. This proves that ${y}_{1}(\mathrm{\infty})=0$.

Since $\lambda \ge 1$, then using the change of the order of integration, we get a contradiction for large *t*. This proves that ${y}_{1}(\mathrm{\infty})>0$. □

*Proof of Theorem 1*In view of (11), (2) is disconjugate on ${\mathbb{R}}_{+}$. By Proposition 1, equation (1) has a solution

*x*satisfying (4). Therefore, system (10) has a solution such that ${y}_{i}(t)>0$ and ${y}_{i}^{\mathrm{\prime}}(t)<0$ for $t\in {\mathbb{R}}_{+}$. Choose

*h*in (10) as a principal solution of (2). The Euler equation

for large *t*; see, *e.g.*, [11]. Thus there exists $\ell >0$ such that $\ell \le h(t)\le \ell \sqrt{t+1}$ for $t\ge 0$. Assume (12). Then (15) holds, and by Lemma 1 a solution *x* satisfies (3).

Assume (13). Then the principal solution *h* of (2) satisfies $h(t)\sim \ell $ for large *t* (see, *e.g.*, [11]). Hence, condition (15) reads as (14), and by Lemma 1 this condition is equivalent to the property (3). □

As a consequence of Lemma 1, we get the following result.

**Corollary 1**

*Let*(2)

*be disconjugate on*$[0,\mathrm{\infty})$,

*and*$r(t)<0$

*for*$t\in {\mathbb{R}}_{+}$.

*Then any solution*

*x*

*of*(1)

*satisfying*

*is a solution of the Kneser problem*, *i*.*e*., ${(-1)}^{i}{x}^{(i)}(t)>0$ *for* $t\ge 0$ *and* $i=1,2$.

*Proof* Let *h* be a positive solution on ${\mathbb{R}}_{+}$ satisfying (6), and let *x* be a solution of (1) satisfying (18). Then $y=({y}_{1},{y}_{2},{y}_{3},{y}_{4})$, where ${y}_{1}$ are defined by (9), is a solution of system (10). Since ${y}_{1}(t)>0$ for $t\ge 0$ and (6) holds, we have by the Kiguradze lemma (see, *e.g.*, [1]) that either ${y}_{i}^{\mathrm{\prime}}(t)>0$ or ${y}_{i}^{\mathrm{\prime}}(t)<0$ for $i=1,2,3$ and large *t*, say for $t\ge a\ge 0$. Since *x* is positive and tends to zero, we have ${y}_{1}^{\mathrm{\prime}}\le 0$ for $t\ge a$, so also ${y}_{i}^{\mathrm{\prime}}\le 0$ ($i=2,3$) for $t\ge a$. By Lemma 1, we get ${y}_{i}^{\mathrm{\prime}}(\mathrm{\infty})=0$ ($i=2,3$) for $t\ge a$. Since $x(t)>0$ for $t\ge 0$, we have ${y}_{4}^{\mathrm{\prime}}(t)<0$ for $t\ge 0$ and ${y}_{4}$ is positive and decreasing on ${\mathbb{R}}_{+}$. Hence, proceeding by the same argument, ${y}_{i}$ ($i=2,3$) is positive and decreasing on ${\mathbb{R}}_{+}$. Now the conclusion follows from (9). □

### 2.2 Case $r(t)>0$

First we show that the sign condition posed on *r* is necessary for the solvability of problem (1), (4).

A function *g*, defined in a neighborhood of infinity, is said to change sign if there exists a sequence $\{{t}_{k}\}\to \mathrm{\infty}$ such that $g({t}_{k})g({t}_{k+1})<0$.

**Theorem 2**

*Let*$r(t)>0$

*for large*

*t*.

*Then problem*(1), (4)

*has no solution and the following hold*:

- (a)
*If*(2)*is nonoscillatory*,*then every nonoscillatory solution**x**of*(1)*satisfies*$x(t){x}^{\mathrm{\prime}}(t)>0$*and*${x}^{\u2033}$*is of one sign for large**t*. - (b)
*If*(2)*is oscillatory*,*then every nonoscillatory solution**x**of*(1)*satisfies either*$x(t){x}^{\mathrm{\prime}\mathrm{\prime}}(t)\le 0$,*or*${x}^{\mathrm{\prime}\mathrm{\prime}}(t)$*changes sign*.*In addition*,*if a solution**x**satisfies*(3),*then*${x}^{\mathrm{\prime}\mathrm{\prime}}$*changes sign*.

*Proof*Claim (a). Let

*x*be a positive solution of (1) on $[a,\mathrm{\infty})$, or, equivalently, of (5) on $[a,\mathrm{\infty})$, where

*h*satisfies (6). Denote

Letting $t\to \mathrm{\infty}$, we get a contradiction with the positiveness of ${y}_{3}$. The remaining case ${y}_{3}(t)<0$ can be eliminated in a similar way using (6). Observe that system (20) is a special case of the Emden-Fowler system investigated in [13], and the proof follows also from [[13], Lemma 2.1].

*x*of (1) such that $x(t)>0$ and ${x}^{\mathrm{\prime}\mathrm{\prime}}(t)\ge 0$ on $[T,\mathrm{\infty})$, $T\ge 0$. Borůvka [18] proved that if (2) is oscillatory, then there exists a function $\alpha \in {C}^{3}[T,\mathrm{\infty})$, called a

*phase function*, such that ${\alpha}^{\mathrm{\prime}}(t)>0$ and

*X*becomes eventually negative, which is a contradiction. Then $\dot{X}(s)\ge 0$ and $X(s)$ is nondecreasing. Let ${T}_{1}\ge {T}^{\ast}$ be such that $X(s)>0$ on $[{T}_{1},\mathrm{\infty})$. Thus, using (23) we obtain

Hence, ${lim}_{s\to \mathrm{\infty}}\dot{X}(s)=-\mathrm{\infty}$, which contradicts the nonnegativity of $\dot{X}(s)$. Finally, the case $X(s)\equiv 0$ on $[{T}^{\ast},\mathrm{\infty})$ cannot occur, because if ${x}^{\mathrm{\prime}\mathrm{\prime}}(t)\equiv 0$ on $[T,\mathrm{\infty})$, then from (1) and $r(t)>0$, we have $x\equiv 0$ on $[T,\mathrm{\infty})$, which is a contradiction.

Finally, let *x* be a positive solution of (1) satisfying (3). Then ${x}^{\mathrm{\prime}\mathrm{\prime}}$ is either oscillatory or ${x}^{\mathrm{\prime}\mathrm{\prime}}(t)<0$ for large *t*. Assume ${x}^{\mathrm{\prime}\mathrm{\prime}}(t)<0$ on some $J=[T,\mathrm{\infty})$, then ${x}^{\prime}$ is decreasing and either ${x}^{\prime}(t)\ge 0$ or ${x}^{\prime}(t)<0$ for large *t*. If ${x}^{\prime}(t)\ge 0$ for large *t*, then we get a contradiction with (3). If ${x}^{\prime}(t)<0$, then ${x}^{\prime}(t)\le {x}^{\prime}({T}_{1})<0$ for $t\ge {T}_{1}\ge T$ and *x* becomes negative for large *t*. Hence ${x}^{\mathrm{\prime}\mathrm{\prime}}$ must be oscillatory. □

For $\lambda >1$, the analogous result to Theorem 1 is the following oscillation result.

**Proposition 2** *Let* $\lambda >1$, $r(t)>0$ *for large* *t*. *Assume either* (11) *for large* *t*, (12), *or* (13), (14). *Then all the solutions of* (1) *are oscillatory*.

*Proof* Let *x* be a solution of (1) and *h* be the principal solution of (2). Then $y=({y}_{1},{y}_{2},{y}_{3},{y}_{4})$, where ${y}_{i}$ are given by (19), is a solution of system (20). Proceeding by the similar way as in the proof of Theorem 1, we have that (15) holds. Using the change of the order of integration in (15), we can check that conditions of Theorem 4.3 in [13] applied to system (20) are verified. Hence by this result all the solutions of (20) are oscillatory, which gives the conclusion. □

The following result follows from [[7], Theorem 1.5] and completes Proposition 2 in the case when (2) is oscillatory.

**Proposition 3** *Let* $\lambda >1$, $q(t)\equiv 1$ *and* $r(t)>0$ *for* $t\in {\mathbb{R}}_{+}$. *Then the condition* ${\int}^{\mathrm{\infty}}tr(t)\phantom{\rule{0.2em}{0ex}}dt=\mathrm{\infty}$ *is necessary and sufficient for every solution of* (1) *to be oscillatory*.

In the light of these results, in the sequel, we study asymptotic and oscillation problems to (1) when (2) is oscillatory.

## 3 Vanishing at infinity solutions

In this section we study when all nonoscillatory solutions of (1) are vanishing at infinity.

**Theorem 3**

*Let*$\lambda >1$

*and*(2)

*be oscillatory*.

*Assume that*$q(t)\ge K{t}^{-2}$

*for large*

*t*

*and some*$K>0$,

*the functions*

*and*

*Then any eventually positive solution of* (1) *is vanishing at infinity*.

The proof of Theorem 3 is based on the following auxiliary results.

where ${Q}_{i}$ and *R* are continuous functions on $[0,\mathrm{\infty})$. In [[15], Theorem 2.4], the following uniform estimate for positive solutions of (26) with a common domain was proved.

**Proposition 4** ([[15], Theorem 3.4, Corollary 3.6])

*Assume*$\lambda >1$.

*Let*

*y*

*be a positive solution of*(26)

*defined on*$[0,b]$

*and*

*on*$[0,b]$

*for some constants*${r}_{\ast}>0$

*and*$Q>0$.

*Then there exists a positive constant*$M=M(\lambda )$

*such that*

*where*

**Remark 1** In [[15], Theorem 3.4] the constant *M* is explicitly calculated.

**Lemma 2**

*Let*$\lambda >1$.

*Assume that*(27)

*holds on*$[0,\mathrm{\infty})$.

*Then any positive solution of*(26)

*defined on*$[0,\mathrm{\infty})$

*satisfies*

*where* *α* *and* *M* *are constants from Proposition * 4.

*Proof*Let $b\ge \alpha $. By Proposition 4, applied on $[0,b]$, we have $\delta =\delta (s)\equiv \alpha $ for $s\in [\alpha ,b-\alpha ]$ and

Letting $b\to \mathrm{\infty}$, we get (29). □

The next lemma describes the transformation between solutions of (1) and a certain quasi-linear equation.

**Lemma 3**

*Let*$q(t)>0$

*on*$[a,\mathrm{\infty})$

*be such that*

*and consider the transformation*

*Then*$x=x(t)$

*is a solution of equation*(1)

*on*$[a,\mathrm{\infty})$

*if and only if*$y=y(s)$

*is a solution of the equation*

*where* $t=t(s)$ *is the inverse function to* $s=s(t)$.

*Proof*We have

Substituting into (1), we get the conclusion. □

*Proof of Theorem 3*Let

*x*be a positive solution of (1) on $I=[a,\mathrm{\infty})$ ($a>0$). Suppose, for simplicity, that $q(t)\ge K{t}^{-2}$ for $t\ge a$. Let

*i.e.*,

*Q*is defined by (31) and (32). Choose ${t}_{0}\ge T$ arbitrarily. We apply Lemma 2 to equation (30) with

where $C=M{\alpha}^{-\frac{4}{\lambda -1}}$. Letting ${t}_{0}\to \mathrm{\infty}$, we have by (35) that ${t}^{\ast}({t}_{0})\to \mathrm{\infty}$ and the conclusion follows from (25) and (37). □

From the proof of Theorem 3, we get the estimate for the set of all nonoscillatory solutions of (1) which will be used in the next section.

**Corollary 2**

*Let*$\lambda >1$, ${lim}_{t\to \mathrm{\infty}}q(t)=\mathrm{\infty}$, (24)

*and*(25)

*hold*.

*Then*,

*for any*$\epsilon >0$,

*there exists a positive constant*$C=C(\lambda ,q(t),\epsilon )$

*and*$T\ge 0$

*such that every nonoscillatory solution*

*x*

*of*(1)

*satisfies*

*Proof*Let $\epsilon >0$ be fixed and let $T\ge 0$ be such that

*α*is given by (33). Let $t\ge T$ be fixed. Using estimate (37) with ${t}_{0}=t\ge T$, we have

*i.e.*,

Therefore ${t}^{\ast}(t)\ge t-\epsilon $ and estimate (38) follows from (25) and (39). □

**Example 1**Consider the equation

Then $r/{q}^{2}\to \mathrm{\infty}$ and by Theorem 3 all eventually positive solutions are vanishing at infinity. One can check that $x=\frac{1}{t+1}$ is such a solution of (40).

**Open problem** It is an open problem to find conditions for the solvability of boundary value problem (1), (3), (4) in case $r(t)<0$ and (2) is oscillatory.

In view of Theorem 2, Corollary 2 and Proposition 1, it is a question whether (1) can have vanishing at infinity solutions in case $r(t)>0$ and (2) is oscillatory.

In the next section, we show that under certain additional assumptions the answer is negative.

## 4 Oscillation

Here we consider (1) in case $r(t)>0$ for large *t*. When (2) is nonoscillatory, we have established the oscillation criterion in Proposition 2. When (2) is oscillatory, the following oscillation theorem holds.

**Theorem 4**

*Let*$\lambda >1$, $r(t)>0$

*and assumptions*(24), (25)

*hold*.

*Assume*

*and*

*for some* $\epsilon >0$ *and* $\sigma >0$. *Then problem* (1), (3) *is not solvable and all the solutions of* (1) *are oscillatory*.

*Proof*Suppose that (25) holds on $[a,\mathrm{\infty})$. First, observe that the assumption (42) implies that

*x*of (1) such that $x(t)>0$ for $t\ge {t}_{0}\ge 0$. According to Corollary 2, there exists ${\overline{t}}_{0}$ such that

*F*is increasing for large

*t*. Hence, there exists ${t}_{2}\ge {t}_{1}$ such that either

According to Theorem 2(b), ${x}^{\mathrm{\prime}\mathrm{\prime}}$ oscillates. Define by ${\{{\tau}_{k}\}}_{k=1}^{\mathrm{\infty}}$ an increasing sequence of zeros of ${x}^{\mathrm{\prime}\mathrm{\prime}}$ tending to ∞ with ${\tau}_{1}\ge {t}_{2}$.

*Z*is well defined and

we get $Z(t)\le Z({\tau}_{1})<0$ for $t\ge {\tau}_{1}$. This is a contradiction with (49), so (45) is impossible.

If (46) holds, then ${Z}^{\prime}(t)>0$ and ${lim}_{t\to \mathrm{\infty}}Z(t)=\mathrm{\infty}$. This is again a contradiction with (49), so also this case is impossible. □

**Example 2**Consider the equation

where $\sigma =\pm 1$. If $\sigma =-1$ and $c\in (0,1/4)$, then by Theorem 1 this equation has a solution satisfying (3) and (4). If $\sigma =\pm 1$ and $c>1/4$, then by Theorem 3 any nonoscillatory solution (if any) satisfies (3).

## 5 Extensions

*q*,

*r*are as for (1) and $f(u)u>0$ for $u\ne 0$ such that

for some $\lambda \ge 1$ and $k>0$. The prototype of such an extension is the function $f(u)={e}^{u}-1$ for $u\ge 0$.

Theorems 1-4 read for (1′) as follows.

**Theorem 1′** *Let* $\lambda \ge 1$, $r(t)<0$ *and* (11) *hold for* $t\in {\mathbb{R}}_{+}$. *Assume that either* (i) (12), *or* (ii) (13) *and* (14) *hold*. *Then problem* (1′), (3), (4) *has a solution for any* $c>0$.

*Proof of Theorem 1′* It is analogous to the proofs of Proposition 1 and Theorem 1 replacing the nonlinearity ${|{y}_{1}(t)|}^{\lambda}(t)sgn{y}_{1}(t)$ in system (10) by $f({y}_{1}(t))$. Lemma 1 remains to hold as a sufficient condition for (3). □

**Theorem 2′** *Theorem * 2 *remains to hold for* (1′) *without assuming* (50).

*Proof of Theorem 2′* In the proof of claim (a) of Theorem 2, we consider system (20) where the nonlinearity ${|{y}_{1}(t)|}^{\lambda}(t)sgn{y}_{1}(t)$ is replaced by $f({y}_{1}(t))$. The proof of claim (b) of Theorem 2 is the same for the nonlinearity *f*. □

**Theorem 3′** *Theorem * 3 *remains to hold for* (1′).

*Proof of Theorem 3′*Let

*x*be a positive solution of (1′) on $[a,\mathrm{\infty})$. Then $v=x$ is a solution of the equation

Now we apply Theorem 3 to (51). □

**Theorem 4′** *Let the assumptions of Theorem * 4 *hold*. *Then* (1′) *has no eventually positive solutions*.

*Proof of Theorem 4′* It is similar to the one of Theorem 4. In view of (52), the estimate (38) holds and the energy function *F* is the same. □

## Notes

### Acknowledgements

Supported by the grant GAP 201/11/0768 of the Czech Grant Agency.

### References

- 1.Kiguradze I, Chanturia TA:
*Asymptotic Properties of Solutions of Nonautonomous Ordinary Differential Equations*. Kluwer Academic, Dordrecht; 1993.CrossRefGoogle Scholar - 2.Mawhin J, Zanolin F: A continuation approach to fourth order superlinear periodic boundary value problems.
*Topol. Methods Nonlinear Anal.*1993, 2(1):55-74.MathSciNetGoogle Scholar - 3.Gupta C, Mawhin J: Weighted eigenvalue, eigenfunctions and boundary value problems for fourth order ordinary differential equations. World Sci. Ser. Appl. Anal. 1. In
*Recent Trends in Differential Equations*. World Scientific, River Edge; 1992:253-267.CrossRefGoogle Scholar - 4.Ahlbrandt CD, Hinton DB, Lewis R: The effect of variable change on oscillation and disconjugacy criteria with applications to spectral theory and asymptotic theory.
*J. Math. Anal. Appl.*1981, 81: 234-277. 10.1016/0022-247X(81)90060-3MathSciNetCrossRefGoogle Scholar - 5.Agarwal RP, O’Regan D:
*Infinite Interval Problems for Differential, Difference and Integral Equations*. Kluwer Academic, Dordrecht; 2001.CrossRefGoogle Scholar - 6.Elias U 396. In
*Oscillation Theory of Two-Term Differential Equations*. Kluwer Academic, Dordrecht; 1997.CrossRefGoogle Scholar - 7.Kiguradze I: An oscillation criterion for a class of ordinary differential equations.
*Differ. Uravn. (Minsk)*1992, 28: 201-214.MathSciNetGoogle Scholar - 8.Bartušek M, Cecchi M, Došlá Z, Marini M: Asymptotics for higher order differential equations with a middle term.
*J. Math. Anal. Appl.*2012, 388: 1130-1140. doi:10.1016/j.jmaa.2011.10.059 10.1016/j.jmaa.2011.10.059MathSciNetCrossRefGoogle Scholar - 9.Bartušek M, Cecchi M, Došlá Z, Marini M: Fourth-order differential equation with deviating argument.
*Abstr. Appl. Anal.*2012., 2012: Article ID 185242Google Scholar - 10.Berchio E, Ferrero A, Gazzola F, Karageorgis P: Qualitative behavior of global solutions to some nonlinear fourth order differential equations.
*J. Differ. Equ.*2011, 251: 2696-2727. 10.1016/j.jde.2011.05.036MathSciNetCrossRefGoogle Scholar - 11.Hartman P:
*Ordinary Differential Equations*. Wiley, New York; 1964.Google Scholar - 12.Chanturia TA: On monotone solutions of a system of nonlinear differential equations.
*Ann. Pol. Math.*1980, 37: 59-70. (in Russian)Google Scholar - 13.Kusano T, Naito M, Wu F: On the oscillation of solutions of 4-dimensional Emden-Fowler differential systems.
*Adv. Math. Sci. Appl.*2001, 11(2):685-719.MathSciNetGoogle Scholar - 14.Naito M, Wu F: A note on the existence and asymptotic behavior of nonoscillatory solutions of fourth order quasilinear differential equations.
*Acta Math. Hung.*2004, 102: 177-202.MathSciNetCrossRefGoogle Scholar - 15.Astashova IV: Uniform estimates for positive solutions of quasi-linear ordinary differential equations.
*Izv. Ross. Akad. Nauk, Ser. Mat.*2008, 72(6):85-104. (Russian); translation in Izv. Math. 72(6), 1141-1160 (2008)MathSciNetCrossRefGoogle Scholar - 16.Chanturia TA: On singular solutions of nonlinear systems of ordinary differential equations.
*Colloq. Math. Soc. János Bolyai*1976, 15: 107-119.Google Scholar - 17.Bartušek M, Došlá Z: Remark on Kneser problem.
*Appl. Anal.*1995, 56(3-4):327-333. 10.1080/00036819508840329MathSciNetCrossRefGoogle Scholar - 18.Borůvka O:
*Linear Differential Transformationen 2. Ordung*. VEB, Berlin; 1967.Google Scholar

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