Abstract

In this article, we give conditions on parameters k, l that the generalized eigenvalue problem x″″ + kx″ + lx = λh(t)x, 0 < t < 1, x(0) = x(1) = x′(0) = x′(1) = 0 possesses an infinite number of simple positive eigenvalues { λ k } k = 1 ∞ and to each eigenvalue there corresponds an essential unique eigenfunction ψ k which has exactly k - 1 simple zeros in (0,1) and is positive near 0. It follows that we consider the fourth-order two-point boundary value problem x″″ + kx″ + lx = f(t,x), 0 < t < 1, x(0) = x(1) = x′(0) = x′(1) = 0, where f(t, x) ∈ C([0,1] × ℝ, ℝ) satisfies f(t, x)x > 0 for all x ≠ 0, t ∈ [0,1] and lim |x|→0 f(t,x)/x = a(t), lim |x|→+∞ f(t,x)/x = b(t) or lim x→-∞ f(t,x)/x = 0 and lim x→+∞ f(t,x)/x = c(t) for some a(t), b(t), c(t) ∈ C([0,1], (0,+∞)) and t ∈ [0,1]. Furthermore, we obtain the existence and multiplicity results of nodal solutions for the above problem. The proofs of our main results are based upon disconjugate operator theory and the global bifurcation techniques.MSC (2000): 34B15.

Highlights

  • The deformations of an elastic beam in equilibrium state with fixed both endpoints can be described by the fourth-order boundary value problem x + lx = λh(t)f (x), 0 < t < 1, (1:1)x(0) = x(1) = x (0) = x (1) = 0, where f: R ® R is continuous, l Î R is a parameter and l is a given constant

  • When l ≠ 0, l satisfying (H1) and h(t) satisfying (H2), Xu and Han [6] studied the existence of nodal solutions of the problem (1.1) by applying bifurcation techniques, where (H1) l Î (-π4, π4/64) is given constant. (H2) h Î C([0,1], [0, ∞)) with h(t) ≢ 0 on any subinterval of [0,1]

  • Motivated by [6], we consider the existence of nodal solutions of general fourthorder boundary value problem x + kx + lx = f (t, x), 0 < t < 1, (1:2)

Read more

Summary

Introduction

When l ≠ 0, l satisfying (H1) and h(t) satisfying (H2), Xu and Han [6] studied the existence of nodal solutions of the problem (1.1) by applying bifurcation techniques, where (H1) l Î (-π4, π4/64) is given constant. In order to use bifurcation technique to study the nodal solutions of the problem (1.2), we first prove that the generalized eigenvalue problem x + kx + lx = λh(t)x, 0 < t < 1,. For other results on the existence and multiplicity of positive solutions and nodal solutions for the boundary value problems of fourth-order ordinary differential equations based on bifurcation techniques, see [9,10,11,12,13,14]s and their references

Preliminary results Let
From the fact
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.