Abstract

For the pair of functional equations urn:x-wiley:01611712:media:ijmm174267:ijmm174267-math-0001 and urn:x-wiley:01611712:media:ijmm174267:ijmm174267-math-0002 sufficient conditions have been found to cause all solutions of equation (A) to be oscillatory. These conditions depend upon a positive solution of equation (B).

Highlights

  • (r(t)y’(t))’ p(t)h(y(g(t))) 0 sufficient conditions have been found to cause all solutions of equation (A) to be oscillatory

  • The failure in study of equation (i.i) leads us to this work in which we present a different approach to study the oscillation of equation (i.I) which may be sublinear, superlinear, retarded or advanced

  • Graef and Spikes [i], Hammett [2], Kusano and Onose [5,6], Philos and Starkos [7], this author [i0,ii] have studied asymptotic nonoscillation with regard to equation (i.i)

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Summary

Introduction

For the pair of functional equations (A) (r(t)y’(t))’ p(t)h(y(g(t))) 0 sufficient conditions have been found to cause all solutions of equation (A) to be oscillatory. These conditions depend upon a positive solution of equation (B). In this work, is to seek the oscillatory behavior of the equation Rankin [8] presented a new approach to study the oscillatory behavior of the ordinary differential equation y’’(t) + p(t)y(t) f(t), (1.5)

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