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Explicit criteria for the oscillation of secondorder differential equations with several sublinear neutral coefficients
Advances in Difference Equations volume 2020, Article number: 643 (2020)
Abstract
In this work, we present sufficient conditions for oscillation of all solutions of a secondorder functional differential equation. We consider two special cases when \(\gamma >\beta \) and \(\gamma <\beta \). This new theorem complements and improves a number of results reported in the literature. Finally, we provide examples illustrating our results and state an open problem.
1 Introduction
Delay differential equations are widely used in mathematical modeling to describe physical and biological systems, often inducing oscillatory behavior [1–4, 8, 13, 14, 17, 18, 24–26, 28–35].
In the literature, numerous mathematical models with different levels of complexity have been proposed for delay differential equations in order to represent the cardiovascular system (CVS).
The pioneering and remarkable paper of Ottesen [27] shows how to use delay differential equations to solve a cardiovascular model that has a discontinuous derivative. Ottesen [27] also illustrated that complex dynamic interactions between nonlinear behaviors and delays associated with the autonomiccardiac regulation may cause instability [5].
Moreover, a modelbased approach to stability analysis of autonomiccardiac regulation was studied in [5]; specifically, it is important to underline that the autonomiccardiac regulation operates by the interaction between autonomic nervous system (ANS) and cardiovascular system (CVS) [5].
It is clear that mathematical analysis based on physicsbased models can be a versatile tool in examining delay differential equations from the point of view of biological systems.
In this article we consider the neutral differential equation
where \(w(t)=x(t)+\sum_{i=1}^{m}p_{i}(t)x^{\alpha _{i}} (\varsigma _{i}(t) )\), \(\alpha _{i}\) for \(i=1,2,\ldots ,m\), γ and β are the quotients of odd positive integers. Throughout this work, we suppose that:

(A1)
\(\vartheta , \varsigma _{i} \in C([t_{0},\infty ),\mathbb{R}_{+})\), \(\varsigma _{i} \in C^{2}([t_{0},\infty ),\mathbb{R}_{+})\), \(\vartheta (t)< t\), \(\varsigma _{i}(t)< t\), \(\lim_{t\to \infty }\vartheta (t)=\infty \), \(\lim_{t\to \infty }\varsigma _{i}(t)=\infty \) for all \(i=1,2,\ldots \) .

(A2)
\(r\in C^{1}([t_{0},\infty ),\mathbb{R}_{+})\), \(q \in C([t_{0},\infty ),\mathbb{R}_{+})\); \(0\leq q(t)\) for all \(t\geq 0\); \(q(t)\) is not identically zero in any interval \([b,\infty )\).

(A3)
\(\lim_{t\to \infty }R(t)=\infty \), where \(R(t)=\int _{t_{1}}^{t} r^{1/\gamma }(s) \,ds\).

(A4)
\(p_{i} : [t_{0},\infty ) \to \mathbb{R}^{+}\) are continuous functions for \(i=1,2,\ldots ,m\).
In 1978, Brands [11] proved that, for each bounded delay \(\vartheta (t)\), the equation
is oscillatory if and only if the equation
is oscillatory. In [12, 15] Chatzarakis et al. considered a more general equation
and established new oscillation criteria for (2) when \(\lim_{t\to \infty }R(t)=\infty \) and \(\lim_{t\to \infty }R(t)<\infty \).
Wong [37] obtained the oscillation conditions of
in which the neutral coefficient and delays are constants. However, we have seen in [6, 16] that the authors Baculǐkovǎ and Džurina studied
and established the oscillation of solutions of (3) using comparison techniques when \(\gamma =\beta =1\), \(0\leq {}p(t)<\infty \) and \(\lim_{t\to \infty }R(t)=\infty \). In the same technique, Baculikova and Džurina [7] considered (3) and obtained oscillation conditions of (3) by considering the assumptions \(0\leq {}p(t)<\infty \) and \(\lim_{t\to \infty }R(t)=\infty \). In [36], Tripathy et al. studied (3) and established several conditions of the solutions of (3) by considering the assumptions \(\lim_{t\to \infty }R(t)=\infty \) and \(\lim_{t\to \infty }R(t)<\infty \) for different ranges of the neutral coefficient p. In [9], Bohner et al. obtained sufficient conditions for oscillation of solutions of (3) when \(\gamma =\beta \), \(\lim_{t\to \infty }R(t)<\infty \), and \(0 \leq p(t)<1\). Grace et al. [19] studied the oscillation of (3) when \(\gamma =\beta \) and by considering the assumptions \(\lim_{t\to \infty }R(t)<\infty \), \(\lim_{t\to \infty }R(t)=\infty \), and \(0 \leq p(t)<1\). In [22], Li et al. established sufficient conditions for the oscillation of the solutions of (3) under the assumptions \(\lim_{t\to \infty }R(t)<\infty \) and \(p(t) \geq 0\). Karpuz and Santra [21] considered the equation
by considering the assumptions \(\lim_{t\to \infty }R(t)<\infty \) and \(\lim_{t\to \infty }R(t)=\infty \) for different ranges of p.
In fact, equation (1) (that is, halflinear/Emden–Fowler differential equation) arises in a variety of real world problems such as in the study of nonNewtonian fluid theory, the turbulent flow of a polytrophic gas in a porous medium [10, 23]. Neutral differential equations have several applications in the natural sciences and engineering. For example, they often appear in models biological (see, e.g., [20]). In this paper, we restrict our attention to studying oscillation and nonoscillation of (1).
2 Preliminary results
To simplify our notation, for any function \(\rho : [t_{0}, \infty ) \to \mathbb{R}^{+}\) which is positive, continuous decreasing to zero, we set
We need the following lemmas for our work in the sequel.
Lemma 2.1
([20])
If a and b are nonnegative, then
where equality holds if and only if \(a = b\).
Lemma 2.2
Let (A1)–(A4) hold for \(t\geq t_{0}\). If x is an eventually positive solution of (1), then w satisfies
Proof
Let x be an eventually positive solution of (1). Hence, \(w(t)>0\), and there exists \(t_{0} \geq 0\) such that \(x(t)>0\), \(x(\varsigma _{i}(t))>0\), and \(x (\vartheta (t) )>0\) for all \(t\geq t_{0}\) and for all \(i=1,2,\ldots \) . From (1) it follows that
Therefore, \(r(t) (w'(t) )^{\gamma }\) is nonincreasing for \(t\geq t_{0}\). Assume that \(r(t) (w'(t) )^{\gamma }< 0\) for \(t\geq t_{1}>t_{0}\). Hence,
that is,
Using integration from \(t_{1}\) to t, we have
as \(t\to \infty \) due to (A3), which is a contradiction to \(w(t)>0\).
Therefore \(r(t) (w'(t) )^{\gamma }>0\) for all \(t\geq t_{1}\). From \(r(t) (w'(t) )^{\gamma }>0\) and \(r(t)>0\), it follows that \(w'(t)>0\). This completes the proof. □
Lemma 2.3
Let (A1)–(A4) hold for \(t\geq t_{0}\). If x is an eventually positive solution of (1), then w satisfies
and
Proof
Proceeding as in the proof of Lemma 2.2, we obtain (4) for \(t\geq t_{1}\). Since \(r(t) (w'(t) )^{\gamma }\) is decreasing, we have
Again, using the previous inequality, we have
We conclude that \(\frac{w(t)}{R(t)} \) is decreasing for \(t\geq t_{1}\). This completes the proof. □
Lemma 2.4
Let (A1)–(A4) hold for \(t\geq t_{0}\). If x is an eventually positive solution of (1), then w satisfies
Proof
Let x be an eventually positive solution of (1). Hence, \(w(t)>0\), and there exists \(t_{0} \geq 0\) such that
using Lemma 2.1. Since \(w(t)\) is positive and increasing and \(\rho (t)\) is positive and decreasing to zero, there is \(t_{0} \geq t_{1}\) such that
This completes the proof. □
Lemma 2.5
Let (A1)–(A4) hold for \(t\geq t_{0}\). If x is an eventually positive solution of (1), then there exist \(t_{1} > t_{0}\) and \(\delta >0\) such that
hold for all \(t\geq t_{1}\).
Proof
Let x be an eventually positive solution of (1). Then there exists \(t_{0}>0\) such that \(x(t)>0\), \(x(\varsigma _{i}(t))>0\), and \(x (\vartheta (t) )>0\) for all \(t\geq t_{0}\) and for all \(i=1,2,\ldots \) . So, there exists \(t_{1}>t_{0}\) such that Lemma 2.2 holds true and w satisfies (4) for \(t\geq t_{1}\). From \(r(t) (w'(t) )^{\gamma }>0\) and being nonincreasing, we have
Integrating this inequality from \(t_{1}\) to t,
Since \(\lim_{t\to \infty }R(t)=\infty \), there exists a positive constant δ such that (8) holds. On the other hand, \(\lim_{t\to \infty } r(t) (w'(t) )^{\gamma }\) exists, and integrating (1) from t to a, we obtain
Taking limit as \(a\to \infty \),
that is,
Therefore,
This completes the proof. □
3 Sufficient conditions for oscillations
Theorem 3.1
Let (A1)–(A4) hold for \(t\geq t_{0}\). If

(A5)
\(\int _{0}^{\infty }Q_{1}(\eta )\,d\eta =\infty \)
holds, then every solution of (1) is oscillatory.
Proof
Let x be an eventually positive solution of (1). Then there exists \(t_{0}>0\) such that \(x(t)>0\), \(x(\varsigma _{i}(t))>0\), and \(x (\vartheta (t) )>0\) for all \(t\geq t_{0}\) and for all \(i=1,2,\ldots \) . Applying Lemmas 2.2 and 2.4 for \(t\geq t_{1}>t_{0}\), we conclude that w satisfies (4), w is increasing, and \(x(t) \geq P(t)w(t)\) for all \(t\geq t_{1}\). From (1), we have
for \(t\geq t_{1}\). Applying (4), we conclude that \(\lim_{t\to \infty } (r(t) (w'(t) )^{\gamma } )\) exists, and there exist \(t_{2}>t_{1}\) and a number \(c>0\) such that \(w(t) \geq c\) for \(t\geq t_{2}\). Integrating (11) from \(t_{2}\) to t, we have
which is a contradiction to (A5).
The case where x is an eventually negative solution is similar, and we omit it here. Thus, the proof is complete. □
Remark 3.1
Theorem 3.1 holds for any β and γ.
Next, we obtain an oscillation result for equation (1) in the case \(\beta >1\).
Theorem 3.2
Let (A1)–(A4) hold for \(t\geq t_{0}\). If

(A6)
\(\int _{0}^{\infty }Q_{2}(\eta )\,d\eta =\infty \)
holds, then every solution of (1) is oscillatory.
Proof
Proceeding as in the proof of Theorem 3.1, we obtain (11). Applying (7) in (11), we have
The rest of the proof is similar to that of Theorem 3.1, and hence the details are omitted. □
Next, we obtain an oscillation result for equation (1) in the case \(0<\beta <1\).
Theorem 3.3
Let (A1)–(A4) hold for \(t\geq t_{0}\). If

(A7)
\(\int _{0}^{\infty }Q_{3}(\eta )\,d\eta =\infty \)
holds, then every solution of (1) is oscillatory.
Proof
Proceeding as in the proof of Theorem 3.1 we obtain (11). Now (11) can be written as
for \(t\geq t_{2} >t_{1}\). Since \(\frac{w(t)}{R(t)}\) is decreasing, there is a constant k such that
Using (14) and \(\beta <1\) in (13), we have
The rest of the proof is similar to that of Theorem 3.2, and hence it is omitted. □
Next, we assume that there exists a constant \(\beta _{1}\), the quotient of odd positive integers such that \(0<\beta <\beta _{1}<\gamma \).
Theorem 3.4
Let (A1)–(A4) hold for \(t\geq t_{0}\). If

(A8)
\(\int _{0}^{\infty }Q_{4}(\eta ) \,d\eta =\infty \)
holds, then every solution of (1) is oscillatory.
Proof
Let x be an eventually positive solution of (1). So, there exists \(t_{0}>0\) such that \(x(t)>0\), \(x(\varsigma _{i}(t))>0\), and \(x (\vartheta (t) )>0\) for all \(t\geq t_{0}\) and for all \(i=1,2,\ldots \) . Applying Lemmas 2.2 and 2.5 for \(t\geq t_{1}>t_{0}\), we conclude that w satisfies (4), (8), and (9) for all \(t\geq t_{1}\). We can find \(t_{1}>0\) such that
Using (5), (8), \(\beta \beta _{1}<0\), and (15), we have
Since \(U'(t)= q(t)x^{\beta }(\vartheta (t))\leq 0\), \(t\geq t_{2}\), that is, w is nonincreasing, then the last inequality becomes
Therefore,
Integrating (17) from \(t_{2}\) to t and then using the fact that \(U> 0\), we find
which contradicts (A8) as \(t\to \infty \).
This completes the proof. □
Next, we assume that there exists a constant \(\beta _{2}\), the quotient of odd positive integers such that \(\gamma <\beta _{2}<\beta \).
Theorem 3.5
Let (A1)–(A4) hold for \(t\geq t_{0}\), \(\vartheta ^{\prime }(t) \geq \vartheta _{0}>0\) and \(r(t)\) is nondecreasing. If

(A9)
\(\int _{0}^{\infty } [ \frac{1}{r(\eta )}\int _{\eta }^{\infty }Q_{1}( \zeta ) \,d \zeta ]^{1/\gamma } \,d\eta =\infty \)
holds, then every solution of (1) is oscillatory.
Proof
Let x be an eventually positive solution of (1). Then there exists \(t_{0}>0\) such that \(x(t)>0\), \(x(\varsigma _{i}(t))>0\), and \(x (\vartheta (t) )>0\) for all \(t\geq t_{0}\) and \(i=1,2,\ldots \) . Applying Lemmas 2.2 and 2.4 for \(t\geq t_{1}>t_{0}\), we conclude that w satisfies (4), w is increasing, and \(x(t) \geq P(t)w(t)\) for all \(t\geq t_{1}\). So,
implies that
for \(t\geq t_{2}\). From \(r(t) (w'(t) )^{\gamma }\) being nonincreasing and \(\vartheta (t)\leq t\), we have
Using the last inequality in (19) and then dividing by \(r(\vartheta (t))w^{\beta _{2}}(\vartheta (t))>0\), and then operating the power \(1/\gamma \) on both sides, we get
for \(t\geq t_{2}\). Multiplying the lefthand side by \(\vartheta '(t)/\vartheta _{0} \geq 1\) and integrating from \(t_{2}\) to t, we find
Since \(\gamma <\beta _{2}\), \(r(\vartheta (\eta ))\leq r(\eta )\) and
then (20) becomes
which is a contradiction to (A9). This contradiction implies that the solution x cannot be eventually positive. The case where x is eventually negative is very similar, and we omit it here. □
We finalize the paper by presenting some examples to show effectiveness and feasibility of the main results and Remark 3.3.
Example 3.1
Consider the differential equation
where \(r(t) :\equiv y\), \(q(t) :\equiv t^{6}\), \(\vartheta (t) :\equiv \frac{t}{2}\), \(\beta =\gamma =3\), \(p_{i}(t) :\equiv \frac{1}{t^{i}}\), \(\alpha _{i} :\equiv \frac{1}{2i+1}\), and \(\varsigma _{i}(t) :\equiv \frac{t}{i+1}\) for \(i=1,2,\ldots ,m\), and \(t\geq 4\). All the assumptions of Theorem 3.1 can be verified with the index \(i=1,2\) and \(\rho (t)=\frac{1}{t}\). Hence, due to Theorem 3.1 every solution of (21) is oscillatory.
Example 3.2
Consider the differential equation
where \(r(t) :\equiv t \), \(q(t) :\equiv t^{\frac{6}{5}}\), \(\vartheta (t) :\equiv \frac{t}{2}\), \(\beta =1 < \gamma =5\), \(p_{i}(t) :\equiv \frac{1}{t^{i}}\), \(\alpha _{i} :\equiv \frac{1}{2i+1}\), and \(\varsigma _{i}(t) :\equiv \frac{t}{i+2}\) for \(i=1,2,\ldots ,m\) and \(t\geq 2\). All the assumptions of Theorem 3.4 (or Theorem 3.1) can be verified with the index \(i=1,2\) and \(\rho (t)=\frac{1}{t}\). Hence, due to Theorem 3.4 (or Theorem 3.1) every solution of (22) is oscillatory.
Example 3.3
Consider the differential equation
where \(r(t) :\equiv t+1 \), \(q(t) :\equiv t^{12}\), \(\vartheta (t) :\equiv \frac{t}{2}\), \(\vartheta ^{\prime }(t)>\frac{1}{3}=\vartheta _{0}\), \(\beta =3 > \gamma =1\), \(p_{i}(t) :\equiv \frac{1}{t^{2i}}\), \(\alpha _{i} :\equiv \frac{2i1}{2i+1}\), and \(\varsigma _{i}(t) :\equiv \frac{t}{i+1}\) for \(i=1,2,\ldots ,m\) and \(t\geq 2\). All the assumptions of Theorem 3.5 (or Theorem 3.1) can be verified with the index \(i=1,2\) and \(\rho (t)=\frac{1}{t^{2}}\). Hence, due to Theorem 3.4 (or Theorem 3.1), every solution of (23) is oscillatory.
4 Conclusion
In this work, we have undertaken the problem by taking a secondorder nonlinear neutral differential equation with sublinear neutral terms and established the sufficient conditions for oscillation of (1). However, we failed to establish the necessary and sufficient conditions for oscillation of all solutions of (1) by using the method adopted in the current paper. It seems that some other method may be required to establish the necessary and sufficient conditions for oscillation.
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Santra, S.S., Ghosh, T. & Bazighifan, O. Explicit criteria for the oscillation of secondorder differential equations with several sublinear neutral coefficients. Adv Differ Equ 2020, 643 (2020). https://doi.org/10.1186/s13662020031011
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DOI: https://doi.org/10.1186/s13662020031011
MSC
 34C10
 34K11
Keywords
 Oscillation
 Nonoscillation
 Neutral
 Secondorder