Abstract

By employing a well‐known fixed point theorem, we establish the existence of multiple positive solutions for the following fourth‐order singular differential equation Lu = p(t)f(t, u(t), u′′(t)) − g(t, u(t), u′′(t)), 0 < t < 1, α1u(0) − β1u′(0) = 0, γ1u(1) + δ1u′(1) = 0, α2u′′(0) − β2u′′′(0) = 0, γ2u′′(1) + δ2u′′′(1) = 0, with αi, βi, γi, δi ≥ 0 and βiγi + αiγi + αiδi > 0, i = 1,2, where L denotes the linear operator Lu : = (ru′′′)′ − qu′′, r ∈ C1([0,1], (0, +∞)), and q ∈ C([0,1], [0, +∞)). This equation is viewed as a perturbation of the fourth‐order Sturm‐Liouville problem, where the perturbed term g : (0,1)×[0, +∞)×(−∞, +∞)→(−∞, +∞) only satisfies the global Carathéodory conditions, which implies that the perturbed effect of g on f is quite large so that the nonlinearity can tend to negative infinity at some singular points.

Highlights

  • In this paper, we consider the existence of multiple positive solutions for the following fourthorder singular Sturm-Liouville boundary value problem involving a perturbed termLu p t f t, u t, u t − g t, u t, u t, 0 < t < 1, α1u 0 − β1u 0 0, γ1u 1 δ1u 1 0, α2u 0 − β2u 0 0, γ2u 1 δ2u 1 0, 1.1Journal of Applied Mathematics where αi, βi, γi, δi ≥ 0 and βiγi αiγi αiδi > 0, i 1, 2, and L denotes the linear operator Lu : ru − qu, r ∈ C1 0, 1, 0, ∞ and q ∈ C 0, 1, 0, ∞ and q ∈ C 0, 1, 0, ∞

  • It mainly describes the deformation of an elastic beam for g t, u, u ≡ 0; for example, under the Lidstone boundary condition, u 0 u 1 u 0 u 1 0, 1.2 problem 1.1 is used to model such phenomena as the deflection of an elastic beam supported at the endpoints; see 1, 3, 5, 7–11

  • If the boundary condition of 1.1 is a Focal boundary condition, it describes the deflection of an elastic beam having both end-points fixed, or having one end supported and the other end clamped with sliding clamps

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Summary

Introduction

We consider the existence of multiple positive solutions for the following fourthorder singular Sturm-Liouville boundary value problem involving a perturbed termLu p t f t, u t , u t − g t, u t , u t , 0 < t < 1, α1u 0 − β1u 0 0, γ1u 1 δ1u 1 0, α2u 0 − β2u 0 0, γ2u 1 δ2u 1 0, 1.1Journal of Applied Mathematics where αi, βi, γi, δi ≥ 0 and βiγi αiγi αiδi > 0, i 1, 2, and L denotes the linear operator Lu : ru − qu , r ∈ C1 0, 1 , 0, ∞ and q ∈ C 0, 1 , 0, ∞ and q ∈ C 0, 1 , 0, ∞. The perturbed term, g : 0, 1 × 0, ∞ × −∞, ∞ → 0, ∞ , satisfies global Caratheodory’s conditions.

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