International Journal of Analysis and Applications ISSN 2291-8639 Volume 14, Number 2 (2017), 147-154 http://www.etamaths.com OSCILLATION OF NONLINEAR DELAY DIFFERENTIAL EQUATION WITH NON-MONOTONE ARGUMENTS ÖZKAN ÖCALAN1,∗, NURTEN KILIÇ2, SERMIN ŞAHİN3 AND UMUT MUTLU ÖZKAN3 Abstract. Consider the first-order nonlinear retarded differential equation x′(t) + p(t)f (x (τ(t))) = 0, t ≥ t0 where p(t) and τ(t) are function of positive real numbers such that τ(t) ≤ t for t ≥ t0, and limt→∞ τ(t) = ∞. Under the assumption that the retarded argument is non-monotone, new oscillation results are given. An example illustrating the result is also given. Keywords: delay differential equation; non-monotone argument; oscillatory solutions; nonoscil- latory solutions. 2010 Mathematics Subject Classification: 34K11, 34K06. 1. Introduction Consider the nonlinear retarded differential equation x′(t) + p(t)f (x (τ(t))) = 0, t ≥ t0 (1.1) where p(t) and τ(t) are functions of nonnegative real numbers, and τ(t) is non-monotone or nonde- creasing such that τ(t) ≤ t for t ≥ t0, and lim t→∞ τ(t) = ∞, (1.2) and f ∈ C(R,R) and xf(x) > 0 for x 6= 0. (1.3) By a solution of (1.1) we mean a continuously differentiable function defined on [τ(T0),∞] for some T0 ≥ t0 and such that (1.1) is satisfied for t ≥ T0. Such a solution is called oscillatory if it has arbitrarily large zeros. Otherwise, it is called nonoscillatory. Recently there has been an increasing interest in the study of the oscillatory behavior of the following special form of (1.1) x′(t) + p(t)x (τ(t)) = 0, t ≥ t0. (1.4) See, for example, [1−19] and the references cited therein. The first systematic study for the oscilla- tion of all solutions of equation (1.4) was made by Myshkis. In 1950 [17] he proved that every solution of (1.4) oscillates if lim sup t→∞ [t− τ(t)] < ∞ and lim inf t→∞ [t− τ(t)] lim inf t→∞ p(t) > 1 e . In 1972, Ladas, Lakshmikantham and Papadakis [16] proved that the same conclusion holds if, in addition, τ is a non-decreasing function and lim sup t→∞ t∫ τ(t) p(s)ds > 1. (1.5) In 1982, Koplatadze and Canturija [14] established the following result. Received 12th April, 2017; accepted 5th June, 2017; published 3rd July, 2017. 2010 Mathematics Subject Classification. 34K11, 34K06. Key words and phrases. delay differential equation; non-monotone argument; oscillatory solutions; nonoscillatory solutions. c©2017 Authors retain the copyrights of their papers, and all open access articles are distributed under the terms of the Creative Commons Attribution License. 147 148 ÖCALAN, KILIÇ, ŞAHİN AND ÖZKAN If τ(t) is a non-monotone or nondecreasing and lim inf t→∞ t∫ τ(t) p(s)ds > 1 e , (1.6) then all solutions of Eq.(1.4) oscillate, while if lim sup t→∞ t∫ τ(t) p(s)ds < 1 e , (1.7) then the equation (1.4) has a nonoscillatory solution. To the best of our knowledge, there are few papers dealing with the oscillatory behavior of solutions of (1.1), see, for example, [9, 17]. The following theorem was given by Ladde et al. in [17]. THEOREM A. Assume that the f, p and τ in Eq.(1.1) satisfy the following conditions: i) The condition (1.2) holds and let τ(t) be strictly increasing on R+, ii) p(t) is locally integrable and p(t) ≥ 0, a.e.; iii) The condition (1.3) holds and let f be nondecreasing, and lim x→0 x f(x) = N < +∞. Assume further that lim sup t→∞ t∫ τ(t) p(s)ds > N, or lim inf t→∞ t∫ τ(t) p(s)ds > N e . Then every solution of Eq.(1.1) is oscillatory. The following theorem was given by Fukagai and Kusano in [9]. THEOREM B. Suppose that the conditions (1.2) and (1.3) hold. Suppose moreover that lim sup x→0 |x| |f(x)| = λ < ∞. If lim inf t→∞ t∫ τ(t) p(s)ds > λ e , then every solution of Eq.(1.1) is oscillatory. Thus, in this paper, our aim is to obtain some oscillation criteria for all solutions of Eq.(1.1) under the assumption that τ(t) is non-monotone. 2. Main Results In this section, we present a new sufficient conditions for the oscillation of all solutions of Eq.(1.1), under the assumption that the argument τ(t) is non-monotone or nondecreasing. Set h(t) := sup s≤t τ(s), t ≥ 0. (2.1) Clearly, h(t) is nondecreasing, and τ(t) ≤ h(t) for all t ≥ 0. Assume that the f in Eq.(1.1) satisfy the following condition: lim sup x→0 x f(x) = M, 0 ≤ M < ∞. (2.2) OSCILLATION OF NONLINEAR DELAY DIFFERENTIAL 149 Theorem 2.1. Assume that (1.2), (1.3) and (2.2) holds. If τ(t) is non-monotone or nondecreasing, and lim inf t→∞ t∫ τ(t) p(s)ds > M e , (2.3) then all solutions of Eq.(1.1) oscillate. Proof. Assume, for the sake of contradiction, that there exists a nonoscillatory solution x(t) of (1.1). Since −x(t) is also a solution of (1.1), we can confine our discussion only to the case where the solution x(t) is eventually positive. Then there exists t1 > t0 such that x(t), x (τ(t)) > 0, for all t ≥ t1. Thus, from (1.1) we have x′(t) = −p(t)f (x (τ(t))) ≤ 0, for all t ≥ t1. Thus x(t) is nonincreasing and has a limit l ≥ 0 as t →∞. Now, we claim that l = 0. Condition (2.3) implies that ∞∫ a p(t)dt = ∞. (2.4) In view of (2.4) and by the Theorem 3.1.5 in [17] that limt→∞x (t) = 0. Suppose M > 0. Then, in view of (2.2) we can choose t2 > t1 so large that f(x (t)) ≥ 1 2M x(t) for t ≥ t2. (2.5) On the other hand, we know from Lemma 2.1.1 [7] that lim inf t→∞ t∫ h(t) p(s)ds = lim inf t→∞ t∫ τ(t) p(s)ds. (2.6) Since h(t) ≥ τ(t) and x(t) is nonincreasing , by (1.1) and (2.5) we have x′(t) + 1 2M p(t)x(h(t)) ≤ 0, t ≥ t3. (2.7) Also, from (2.3) and (2.6) it follows that there exists a constant c > 0 such that t∫ h(t) p(s)ds ≥ c > M e , t ≥ t3 ≥ t2. (2.8) So, from (2.8), there exists a real number t∗ ∈ (h(t), t), for all t ≥ t3 such that t∗∫ h(t) p(s)ds > M 2e and t∫ t∗ p(s)ds > M 2e . (2.9) Integrating (2.7) from h(t) to t∗ and using x(t) is nonincreasing then we have x(t∗) −x (h(t)) + 1 2M t∗∫ h(t) p(s)x (h(s)) ds ≤ 0, or x(t∗) −x (h(t)) + 1 2M x (h(t∗)) t∗∫ h(t) p(s)ds ≤ 0. Thus, by (2.9), we have −x (h(t)) + 1 2M x (h(t∗)) M 2e < 0. (2.10) 150 ÖCALAN, KILIÇ, ŞAHİN AND ÖZKAN Integrating (2.7) from t∗ to t and using the same facts , we get x(t) −x (t∗) + 1 2M t∫ t∗ p(s)x (h(s)) ds ≤ 0. Thus, by (2.9), we have −x (t∗) + 1 2M x (h(t)) M 2e < 0. (2.11) Combining the inequalities (2.10) and (2.11), we obtain x(t∗) > x (h(t)) 1 4e > x (h(t∗)) ( 1 4e )2 , and hence we have x (h(t∗)) x(t∗) < (4e) 2 for t ≥ t4. Let w = x(h(t∗)) x(t∗) ≥ 1, and because of 1 ≤ w < (4e)2 , w is finite. Now dividing (1.1) with x(t) and then integrating from h(t) to t we obtain t∫ h(t) x′(s) x(s) ds + t∫ h(t) p(s) f(x(τ(s))) x(s) ds = 0 and ln x(t) x(h(t)) + t∫ h(t) p(s) f(x(τ(s))) x(τ(s)) x(τ(s)) x(s) ds = 0 Since x(t) is nonincreasing, we get ln x(t) x(h(t)) + t∫ h(t) p(s) f(x(τ(s))) x(τ(s)) x(h(s)) x(s) ds ≤ 0 and ln x(h(t)) x(t) ≥ f(x(τ(ξ))) x(τ(ξ)) x(h(ξ)) x(ξ) t∫ h(t) p(s)ds, (2.12) where ξ is defined with h(t) < ξ < t, while t −→ ∞, ξ −→ ∞ and because of this h(t) −→ ∞. Then taking lower limit on both side of (2.12), we obtain ln w ≥ w e . But this is impossible since ln x ≤ x e for all x > 0. The case where M = 0 can be discussed similarly. The proof of the theorem is completed. � Theorem 2.2. Assume that (1.2), (1.3), (2.2) and (2.4) holds. If τ(t) is non-monotone, and lim sup t→∞ t∫ h(t) p(s)ds > 2M (2.13) where h(t) is defined by (2.1), then all solutions of Eq.(1.1) oscillate. OSCILLATION OF NONLINEAR DELAY DIFFERENTIAL 151 Proof. Assume, for the sake of contradiction, that there exist a nonoscillatory solution x(t) of (1.1). In view of (2.4), we know from Theorem 2.1 that lim t→∞ x(t) = 0, for t ≥ t1. Considering equation (1.1) x′(t) + p(t)f(x(τ(t))) = 0 by (2.5) we get x′(t) + 1 2M p(t)x(τ(t)) ≤ 0 Since h(t) ≥ τ(t) and x(t) is nonincreasing x′(t) + 1 2M p(t)x(h(t)) ≤ 0 (2.14) Integrating (2.14) from h(t) to t, and using the fact that the function x(t) is nonincreasing and the function h(t) is nondecreasing x(t) −x(h(t)) + 1 2M t∫ h(t) p(s)x(h(s))ds ≤ 0 or x(t) −x(h(t)) + 1 2M x(h(t)) t∫ h(t) p(s)ds ≤ 0 This implies x(t) −x(h(t)) +  1 − 1 2M t∫ h(t) p(s)ds   ≤ 0 and hence t∫ h(t) p(s)ds < 2M for sufficiently t. Therefore, lim sup t→∞ t∫ h(t) p(s)ds ≤ 2M This is a contradiction to (2.13). The proof is completed. � Now, assume that f is nondecreasing function then we have the following result. Theorem 2.3. Assume that (1.2), (1.3), (2.2) and (2.4) hold. If τ(t) is non-monotone, f is nonde- creasing function and lim sup t→∞ t∫ τ(t) p(s)ds > M (2.15) where h(t) is defined by (2.1), then all solutions of Eq.(1.1) oscillate. 152 ÖCALAN, KILIÇ, ŞAHİN AND ÖZKAN Proof. Assume, for the sake of contradiction, that there exist a nonoscillatory solution x(t) of (1.1). In view of (2.4), we know from Theorem 2.1 that lim t→∞ x(t) = 0, for t ≥ t1. Considering equation (1.1) x′(t) + p(t)f(x(τ(t))) = 0 Since τ(t) ≤ h(t), x(t) is nonincreasing and f is nondecreasing we have x′(t) + p(t)f(x(h(t))) ≤ 0 (2.16) Integrating (2.16) from h(t) to t and using the fact that x(t) is nonincreasing and f, h(t) are nondecreasing x(t) −x(h(t)) + t∫ h(t) p(s)f(x(h(s)))ds ≤ 0 or x(t) −x(h(t)) + f(x(h(t))) t∫ h(t) p(s)ds ≤ 0 and so x(t) −x(h(t))  1 − f(x(h(t))) x(h(t)) t∫ h(t) p(s)ds   ≤ 0 Therefore 1 > f(x(h(t))) x(h(t)) t∫ h(t) p(s)ds ≥ 1 M lim sup t→∞ t∫ h(t) p(s)ds That is a contradiction. The proof is completed. � We remark that if τ(t) is nondecreasing, then we have τ(t) = h(t) for all t, and the condition (2.13) and (2.15), respectively, reduce to lim sup t→∞ t∫ τ(t) p(s)ds > 2M (2.16) and lim sup t→∞ t∫ τ(t) p(s)ds > M (2.17) Now, we have the following example. Example 2.1. Consider the nonlinear delay differential equation x′(t) + 1 e x (τ(t)) ln (10 + |x (τ(t))|) = 0, t > 0, (2.18) OSCILLATION OF NONLINEAR DELAY DIFFERENTIAL 153 where τ(t) =   t− 1, if t ∈ [3k, 3k + 1] −3t + 12k + 3, if t ∈ [3k + 1, 3k + 2] 5t− 12k − 13, if t ∈ [3k + 2, 3k + 3] , k ∈ N0. By (2.1), we see that h(t) := sup s≤t τ(s) =   t− 1, if t ∈ [3k, 3k + 1] 3k, if t ∈ [3k + 1, 3k + 2.6] 5t− 12k − 13, if t ∈ [3k + 2.6, 3k + 3] , k ∈ N0. If we put p(t) = 1 e and f(x) = x ln(10 + |x|). Then, we have M = lim sup x→0 x f(x) = lim sup x→0 x x ln(10 + |x|) = 1 ln 10 and lim inf t→∞ ∫ t τ(t) p(s)ds = 1 e > M e = 1 e ln 10 that is, all conditions of Theorem 2.1 are satisfied and therefore all solutions of (2.18) oscillate. References [1] O. Arino, I. Győri and A. Jawhari, Oscillation criteria in delay equations, J. Differential Equations 53 (1984), 115-123. [2] L. Berezansky and E. Braverman, On some constants for oscillation and stability of delay equations, Proc. Amer. Math. Soc. 139 (11) (2011), 4017-4026. [3] E. Braverman, B. Karpuz, On oscillation of differential and difference equations with non-monotone delays, Appl. Math. Comput. 218 (2011) 3880-3887. [4] George E. Chatzarakis and Özkan Öcalan, Oscillations of differential equations with non-monotone retarded argu- ments, LMS J. Comput. Math., 19 (1) (2016) 98–104. [5] A. Elbert and I. P. Stavroulakis, Oscillations of first order differential equations with deviating arguments, Univ of Ioannina T. R. No 172 (1990), Recent trends in differential equations, 163-178, World Sci. Ser. Appl. Anal., 1, World Sci. Publishing Co. (1992). [6] A. Elbert and I. P. Stavroulakis, Oscillation and non-oscillation criteria for delay differential equations, Proc. Amer. Math. Soc., 123 (1995), 1503-1510. [7] L. H. Erbe, Qingkai Kong and B.G. Zhang, Oscillation Theory for Functional Differential Equations, Marcel Dekker, New York, 1995. [8] L. H. Erbe and B. G. Zhang, Oscillation of first order linear differential equations with deviating arguments, Differential Integral Equations, 1 (1988), 305-314. [9] N. Fukagai and T. Kusano, Oscillation theory of first order functional differential equations with deviating argu- ments, Ann. Mat. Pura Appl.,136 (1984), 95-117. [10] K.Gopalsamy, Stability and Oscillations in Delay Differential Equations of Population Dynamics, Kluwer Academic Publishers, 1992. [11] M. K. Grammatikopoulos, R. G. Koplatadze and I. P. Stavroulakis, On the oscillation of solutions of first order differential equations with retarded arguments, Georgian Math. J., 10 (2003), 63-76. [12] I. Győri and G. Ladas, Oscillation Theory of Delay Differential Equations with Applications, Clarendon Press, Oxford, 1991. [13] B. R. Hunt and J. A. Yorke, When all solutions of x′ = ∑ qi(t)x(t−Ti(t)) oscillate, J. Differential Equations 53 (1984), 139-145. [14] R. G. Koplatadze and T. A. Chanturija, Oscillating and monotone solutions of first-order differential equations with deviating arguments, (Russian), Differentsial’nye Uravneniya, 8 (1982), 1463-1465. [15] G. Ladas, Sharp conditions for oscillations caused by delay, Applicable Anal., 9 (1979), 93-98. [16] G. Ladas, V. Laskhmikantham and J.S. Papadakis, Oscillations of higher-order retarded differential equations generated by retarded arguments, Delay and Functional Differential Equations and Their Applications, Academic Press, New York, 1972, 219–231. [17] G.S. Ladde, V. Lakshmikantham, B.G. Zhang, Oscillation Theory of Differential Equations with Deviating Argu- ments, Monographs and Textbooks in Pure and Applied Mathematics, vol. 110, Marcel Dekker, Inc., New York, 1987. [18] A. D. Myshkis, Linear homogeneous differential equations of first order with deviating arguments, Uspekhi Mat. Nauk, 5 (1950), 160-162 (Russian). [19] X.H. Tang, Oscillation of first order delay differential equations with distributed delay, J. Math. Anal. Appl. 289 (2004), 367-378. 154 ÖCALAN, KILIÇ, ŞAHİN AND ÖZKAN 1Akdeniz University, Faculty of Science, Department of Mathematics, 07058, Antalya, Turkey 2Dumlupınar University, Faculty of Science and Arts, Department of Mathematics, 43000, Kütahya, Turkey 3Afyon Kocatepe University, Faculty of Science and Arts, Department of Mathematics, ANS Campus, 03200, Afyon, Turkey ∗Corresponding author: ozkanocalan@akdeniz.edu.tr 1. Introduction 2. Main Results References