Abstract
Consider the first-order linear differential equation with several retarded arguments
where the functions pk, τk ∈ C([t0, ∞), ℝ+), τk(t) < t for t ≥ t0 and limt→∞τk(t) = ∞, for every k = 1, 2, …, n. Oscillation conditions which essentially improve known results in the literature are established. An example illustrating the results is given.
1 Introduction
This paper is concerned with the oscillation of the first order differential equation with several delays of the form
where pk, τk ∈ C([t0, ∞), [0, ∞)), such that
Let T0 ∈ [t0, ∞), τ (t) = min{τk(t) : k = 1, …, n} and τ(−1)(t) = inf{τ (s) : s ≥ t}. By a solution of Eq. (1) we understand a function x ∈ C([t0, ∞), ℝ) continuously differentiable on [τ(−1)(t0), ∞) which satisfies (1) for t ≥ τ(−1)(t0). Such a solution is called oscillatory if it has arbitrarily large zeros, and otherwise it is called nonoscillatory.
We assume throughout this work that there exist t1 ≥ t0, a family of nondecreasing continuous functions
To simplify the notations, we denote by λ (ξ) the smaller root of the equation eξλ = λ, ξ ≥ 0 and
Next, we mention some known oscillation criteria for Eq. (1).
In the case that the arguments τk(t) are monotone the following sufficient oscillation conditions have been established. In 1978, Ladde [1] and in 1982 Ladas and Stavroulakis [2] obtained the sufficient oscillatory criterion
where
In 1984, Hunt and Yorke [3] established the condition
where (t − τk(t)) ≤ τ0, for some τ0 > 0, 1 ≤ k ≤ n.
Also, in 1984, Fukagai and Kusano [4] established the following result.
Assume that there is a continuous nondecreasing functionτ∗ (t)such thatτk(t) ≤ τ∗ (t) ≤ tfort ≥ t0, 1 ≤ k ≤ n. If
then all solutions of Eq. (1)oscillate. If, on the other hand, there exists a continuous nondecreasing functionτ∗ (t) such thatτ∗ (t) ≤ τk(t) fort ≥ t0, 1 ≤ k ≤ n, limt→∞τ∗ (t) = ∞ andfor all sufficiently larget,
thenEq.(1)has a non-oscillatory solution.
In 2003, Grammatikopoulos, Koplatadze and Stavroulakis [5] improved the above results as follows:
Assume that the functionsτkare nondecreasing for allk ∈ {1, …, n,
and
If
then all solutions of Eq. (1)oscillate.
In the case of non-monotone arguments we mention the following known oscillation results. In 2015 Infante, Koplatadze and Stavroulakis [6] obtained the following sufficient oscillation conditions:
and
where
Also, in 2015 Koplatadze [7] derived the following three conditions. The first one takes the form
where k ∈ ℕ and
and
The second condition is
where ϵ ∈ (0, λ (p̄∗)), and
The third condition is
and
In 2016, Braverman, Chatzarakis and Stavroulakis [8] obtained the sufficient condition
where
and
Also, in 2016 Akca, Chatzarakis and Stavroulakis [9] obtained the sufficient condition
where
2 Main results
To obtain our main results we need the following lemmas:
Lemma 2.1
([6]). Let x(t) be an eventually positive solution of Eq. (1). Then
whereqkis defined by(4).
Lemma 2.2
([10]). Assume that
andx(t) is an eventually positive solution of the first order delay differential inequality
whereP ∈ C([t1, ∞), [0, ∞)). If 0 ≤ α* ≤
Theorem 2.3
Assume that
and
where
andϵ ∈ (0, λ (ρ)). Then all solutions of Eq.(1)are oscillatory.
Proof
Assume the contrary, i.e., there exists a nonoscillatory solution x(t) of (1). Because of the linearity of (1), we assume that x(t) is eventually positive. Therefore, there exists a sufficiently large t2 ≥ t1 such that x(τk(t)) > 0, for all t ≥ t2, k = 1, 2, …, n. Thus, equation (1) implies that x(t) is nonincreasing for all t ≥ t2. Integrating (1) from τi(t) to t, we obtain
Also, dividing (1) by x(t) and integrating the resulting equation from τk(s) to gk(t), we get
Substituting this into (10),
Multiplying the above equation by pi(t), and taking the sum over i, it follows that
The substitution
which in turn, by integrating from g(t) to t, leads to
Hence, the nonincreasing nature of y(t) implies that
for all t ≥ t3 and some t3 ≥ t2.
On the other hand, using the nonincreasing nature of x(t), equation (1) implies that
Therefore, from [11, Lemma 2.1.2], we obtain
for some t4 ≥ t3. This together with (12) implies that
for all t ≥ t5, where t5 ≥ t4. That is
for all t ≥ t5. Also, in view of Lemma 2.2, for sufficiently small ϵ∗ > 0 and some t6 ≥ t5, inequality (13) leads to
Therefore,
Combining this inequality with (15), it follows that
Then
Notice that, by integrating (13) from g(t) to t and using the nonincreasing nature of x(t), we obtain
Now, letting ϵ∗ → 0 in (16), we arrive at a contradiction with (9). The proof is complete. □
Remark 2.4
Theorem 2.3 is proved using the core idea of the proof of [12, Theorem 2.1] which is given for Equation (1) when n = 1. However, Theorem 2.3 produces a new oscillation criterion even for equations with only one non-monotone delay.
Using Lemma 2.1 instead of [11, Lemma 2.1.2], similar reasoning as in the proof of Theorem 2.3 implies the following result:
Theorem 2.5
Assume that
where
qℓ is defined by (4), ρ is defined as in Theorem 2.3 and ϵℓ ∈ (0, λ (qℓ)). Then all solutions of Equation (1) oscillate.
Theorem 2.6
Assume that
where βk is defined by (5) with 0 < βk ≤
ρ is defined as in Theorem 2.3 and ϵ ∈ (0, λ(ρ )). Then all solutions of Equation (1) oscillate.
Proof
Let x(t) be a nonoscillatory solution of (1). As usual, we assume that x(t) is an eventually positive solution. Substituting (14) into (11), we obtain
for all t ≥ t2 and some t2 ≥ t1 where ϵ ∈ (0, λ (ρ)) and
and some t3 ≥ t2. Using the relation between arithmetic and geometric mean, it follows that
Taking the product on both sides,
Therefore,
Since
Substituting in (17),
On the other hand, the nonincreasing nature of x(t) and (1) imply that
and hence, by Lemma 2.2, it follows that
for some t4 ≥ t3 and sufficiently small ϵ∗ > 0. This together with (18) leads to
for all t ≥ t4. Consequently,
On the other hand, integrating (1) from gk(t) to t, we get
Then, using the nonincreasing nature of x(t), we obtain
But applying Lemma 2.2 to (19), we obtain
Therefore,
This contradiction completes the proof. □
The following example shows that Theorem 2.3 can be applied but conditions (2), (3) and (6) fail to apply as well as (8) when r = 1.
Example 2.7
Consider the first order delay differential equation
where
Clearly

Equation (21) has the form (1) with p1(t) = a(b + sin (t)), p2(t) = a(b + cos (t)), τ1(t) = t −
Consequently,
Let
Now, using Maple, we get
Choose
which means that
That is, condition (9) of Theorem 2.3 is satisfied and therefore all solutions of Eq. (21) oscillate.
We will show, however, that none of the conditions (2), (3), (6), and (8) (with r = 1) is satisfied. Indeed, notice that
Hence,
On the other hand, since h(t) = g(t), pi(t) ≤ a(b+1) for i = 1, 2, where h(t) is defined by (7), we have
Therefore,
Since λ (ρ) ≈ 1.578422807, then
Therefore, none of conditions (2) and (8) (with r = 1) is satisfied.
Also, since
and
Then,
Then
Therefore,
Finally, since
then
Therefore, condition (6) fails to apply.
Acknowledgement
The authors would like to thank the referees for their valuable comments and suggestions.
References
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© 2018 Attia et al., published by De Gruyter
This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 License.
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