Abstract

Employing a generalized Riccati transformation and integral averaging technique, we show that all solutions of the higher order nonlinear delay differential equation \t\t\ty(n+2)(t)+p(t)y(n)(t)+q(t)f(y(g(t)))=0\\documentclass[12pt]{minimal}\t\t\t\t\\usepackage{amsmath}\t\t\t\t\\usepackage{wasysym}\t\t\t\t\\usepackage{amsfonts}\t\t\t\t\\usepackage{amssymb}\t\t\t\t\\usepackage{amsbsy}\t\t\t\t\\usepackage{mathrsfs}\t\t\t\t\\usepackage{upgreek}\t\t\t\t\\setlength{\\oddsidemargin}{-69pt}\t\t\t\t\\begin{document}$$ y^{(n+2)}(t)+p(t)y^{(n)}(t)+q(t)f\\bigl(y\\bigl(g(t)\\bigr)\\bigr)=0 $$\\end{document} will converge to zero or oscillate, under some conditions listed in the theorems of the present paper. Several examples are also given to illustrate the applications of these results.

Highlights

  • The objective of this paper is to investigate the oscillation and asymptotic behavior of solutions to the following higher order nonlinear delay differential equation: y(n+2)(t) + p(t)y(n)(t) + q(t)f (y g(t) = 0, t ∈ I, (1.1)where n is a positive integer, I = [a, +∞) ⊂ R (a ≥ 0)

  • Our attention is restricted to the solutions of equation (1.1) which exist on the interval I and satisfy supt≥T |y(t)| > 0 for any T ≥ a

  • 3 Asymptotic dichotomy we present some sufficient conditions which guarantee that every solution to equation (1.1) oscillates or converges to zero as t approaches to infinity

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Summary

Introduction

In 2014, the oscillation and asymptotic behavior of solutions to the following nonlinear delay differential equation were studied in [15]: x(n+3)(t) + p(t)x(n)(t) + q(t)f x g(t) = 0. The goal of the present paper is to use a generalized method to study the oscillation and asymptotic behavior of solutions to the nonlinear delay differential equation (1.1). We can use the induction method to obtain limt→+∞ y(t) = –∞ This is a contradiction and we finish the proof of Theorem 3.1. Proof Suppose that y(t) is a non-oscillatory solution of equation (1.1) on the interval [T, +∞), where T ≥ a.

Therefore t
We now take ρ and then obtain t
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