Multiple solutions of three-point boundary value problems for second-order impulsive differential equation at resonance

Boundary Value Problems, May 2014

In this paper, by using the coincidence degree theory and the upper and lower solutions method, we deal with the existence of multiple solutions to three-point boundary value problems for second-order differential equation with impulses at resonance. An example is given to show the validity of our results.

Article PDF cannot be displayed. You can download it here:

https://boundaryvalueproblems.springeropen.com/counter/pdf/10.1186/1687-2770-2014-103

Multiple solutions of three-point boundary value problems for second-order impulsive differential equation at resonance

Zhao et al. Boundary Value Problems 2014, 2014:103 http://www.boundaryvalueproblems.com/content/2014/1/103 RESEARCH Open Access Multiple solutions of three-point boundary value problems for second-order impulsive differential equation at resonance Yulin Zhao1* , Haibo Chen2 and Qiming Zhang1 * Correspondence: 1 School of Science, Hunan University of Technology, Zhuzhou, Hunan 412007, PR China Full list of author information is available at the end of the article Abstract In this paper, by using the coincidence degree theory and the upper and lower solutions method, we deal with the existence of multiple solutions to three-point boundary value problems for second-order differential equation with impulses at resonance. An example is given to show the validity of our results. Keywords: resonance; coincidence degree; upper and lower solutions; impulsive; three-point boundary value problems 1 Introduction The purpose of the present paper is to investigate the following second-order impulsive differential equations: ⎧    ⎪ ⎪ ⎨(ρ(t)u (t)) = f (t, u(t), u (t)), t ∈ J, t = tk , u(tk ) = Ik (tk , u(tk )), k = , , . . . , m, ⎪ ⎪ ⎩  u (tk ) = Jk (tk , u(tk )), (.) together with the boundary conditions: u () = , u() = u(η), (.) where J = [, ], ρ : J → (, +∞) is a continuous differentiable function, f : J × R → R is continuous,  < η < , Ik , Jk ∈ C(J, R) for  ≤ k ≤ m, m is a fixed positive integer,  = t < t < t < · · · < tm < tm+ = , η = tk , u(tk ) = u(tk+ ) – u(tk– ) denotes the jump of u(t) at t = tk , u (tk ) = u (tk+ ) – u (tk– ). u (tk+ ), u(tk+ ) (u (tk– ), u(tk– )) represent the right limit (left limit) of u (t) and u(t) at t = tk , respectively. Impulsive differential equations describe processes which experience a sudden change of their state at certain moments. The theory of impulse differential equations has been a significant development in recent years and played a very important role in modern applied mathematical models of real processes rising in phenomena studied in physics, population dynamics, chemical technology, biotechnology, and economics; see [–] and the references therein. ©2014 Zhao et al.; licensee Springer. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. Zhao et al. Boundary Value Problems 2014, 2014:103 http://www.boundaryvalueproblems.com/content/2014/1/103 Page 2 of 17 Recently, several authors (see [, –] and the references therein) have studied the existence of nontrivial or positive solutions for second-order three-point boundary value problem of the type ⎧ ⎨u = f (t, u, u ), ⎩u () = , (.) u() = au(η). Note that the nonlinear term f depends on u and its derivative u , then the relative problem becomes more complicated. A general method to deal with this difficulty is to add some conditions to restrict the growth of the u term. One condition is the Caratheodory nonlinearity, the other usual condition is Nagumo condition or Nagumo-Winter condition (see [, , , –]). When a = , the linear operator Lu = u is invertible, this is the so-called non-resonance case. Gupta et al. made use of the Leray-Schauder continuation theorem to get the results on the existence of the solution for the problems (.) when a =  in []. By using the Leray-Schauder continuation theorem and in the presence of two pairs of upper and lower solutions, Khan and Webb [] established the existence of at least three solutions for the problem (.) when a = . The linear operator Lu = u is non-invertible when a = , this is the so-called resonance case, and the Leray-Schauder continuation theorem cannot be applied. In [], by using the coincidence degree theory of Mawhin [] and some linear or non-linear growth assumptions on f , Feng and Webb obtained the existence of the solution of the problem (.) when a = . By applying the nonlinear alternative of Leray-Schauder, Ma [] have showed the existence of at least one solution for the problem (.) when a = . Recently, using the coincidence degree theory and the concept of autonomous curvature bound set, Liu and Yu [] have studied the existence of at least one solution for the problem (.)-(.) when u(tk ) = Ik (u(tk ), u (tk )), u (tk ) = Jk (u(tk ), u (tk )). In the present paper, we assume that there exist n (n ∈ N and n ≥ ) pairs of upper and lower solutions for problem (.)-(.) and the nonlinear f satisfies a Nagumo-like growth condition with respect to u . By considering a suitably modified nonlinearity and applying the coincidence degree method of Mawhin [], the existence of multiple solutions for the problem (.)-(.) is given. 2 Preliminaries Let   X = PC  (J) ∩ u () = , u() = u(η) , Z = PC(J) × Rm , where       PC(J) = u ∈ C J * , u t – and u t + exist, and u tk– = u(tk ) .   PC  (J) = u : J → R : u(t) is continuously differentiable for t = , , tk ; u t –    and u t + exist, and u tk– = u (tk ) , J * = J\{t , t , . . . , tm }. Obviously, X is a Banach space with the following norm: u X = max sup u(t) , sup u (t) . t∈J t∈J Zhao et al. Boundary Value Problems 2014, 2014:103 http://www.boundaryvalueproblems.com/content/2014/1/103 Page 3 of 17 In the following, we recall the concept of strict upper and lower solutions for problem (.)-(.). Definition . A function α(t) ∈ PC  (J) ∩ C  (J * ) is said to be a strict lower solution of the problem (.)-(.) if   ρ(t)α  (t) > f t, α(t), α  (t) , t ∈ J * ,   α  (tk ) ≥ Jk tk , α(tk ) , α(tk ) = Ik tk , α(tk ) ,  α  () ≥ , (.) k = , , . . . , m, α() – α(η) ≤ . (.) (.) Similarly, a function β(t) ∈ PC  (J) ∩ C  (J * ) is said to be a strict upper solution of the problem (.)-(.) if   ρ(t)β  (t) < f t, β(t), β  (t) , t ∈ J * ,   β  (tk ) ≤ Jk tk , β(tk ) , β(tk ) = Ik tk , β(tk ) ,  β  () ≤ , (.) k = , , . . . , m, β() – β(η) ≥ . (.) (.) Remark . Let f : J × R → R be continuous, Ik , Jk ∈ C(J, R), and u ∈ PC  (J) ∩ C  (J * ) is a solution of the problem (.)-(.), if α(β) is a strict lower solution (strict upper solution) for the problem (.)-(.) with α ≤ u (u ≤ β), then α < u (u < β) on (, ). Definition . Let α be a strict lower solution and β be a strict upper solution for the problem (.)-(.) satisfying α(t) < β(t) on J. We say that f : J × R → R has property (H) relative to α and β, if there exists a function ψ ∈ C  ([, +∞), (, +∞)) such that  f (t, u, p) < ψ |p| , (.) for all u(t) ∈ (–β(t), –α(t)) ∪ (α(t), β(t)), t ∈ J, and +∞  s ds = +∞, θ s + ψ(s) where  ≤ θ < +∞ with |ρ  (t)| ≤ θ , t ∈ J. 3 The key lemmas Let dom L = C  (J * ) ∩ X, and L : dom L → Z, N : u → z,   u → ρ(t)u (t) , u(t ), . . . , u(tm ), u (t ), . (...truncated)


This is a preview of a remote PDF: https://boundaryvalueproblems.springeropen.com/counter/pdf/10.1186/1687-2770-2014-103
Article home page: http://www.boundaryvalueproblems.com/content/2014/1/103

Zhao, Yulin, Chen, Haibo, Zhang, Qiming. Multiple solutions of three-point boundary value problems for second-order impulsive differential equation at resonance, Boundary Value Problems, 2014, pp. 1-17, Volume 2014, Issue 1, DOI: 10.1186/1687-2770-2014-103