Abstract

In this work, we apply Leray-Schauder continuation principle to establish the existence of at least one solution to the third order p-Laplacian boundary value problem on an unbounded domain of the form \begin{equation*} (w(t) \varphi_{p}( u^{\prime\prime}(t)))^{\prime} = K ( t, u(t) , u^{\prime}(t), u^{\prime\prime}(t) ) , t \in ( 0, \infty) \end{equation*} \begin{equation*} u(0)= 0, \, u^{\prime} (0) = \sum^{m}_{i=1} \alpha _{i} \int_{0}^{\xi_{i}} u(t) dt, \, \lim_{t \rightarrow\infty} ( w(t)\varphi_{p} ( u^{\prime \prime} (t)) = 0 \end{equation*} under the nonresonant condition $ \sum_{i=1}^{m} \alpha_{i} \xi^{2} \neq 2. $

Highlights

  • The purpose of this paper is to obtain existence of at least one solution for the third order p-Laplacian boundary value problem (1.1)m ξi u′(0) = αi u(t)dt, u(0) = 0, lim (w(t)φp(u′′(t))) = 0 i=1 t→∞ (1.2)where φp(s) =| s |p−2 s, K : [0, ∞)×R3 → R is a Caratheodory function with respect to L1[0, ∞), αi ∈ R(1 ≤ i ≤ m),0 < ξ1 < ξ2 < ... < ξm < 1 .w(t) > 0, t ∈ [0, ∞), w ∈ C[0, ∞) ∩ C1[0, ∞),1 ∈ L1[0, ∞) and w m i=1 ̸=The condition m i=1is critical since we require a trivial kernel for the differential operator.The boundary value problem (1.1)–(1.2) is said to be at nonresonance

  • In [6] we proved the existence of solutions for the boundary value problem

  • The contribution of this paper is to extend the results of (1.3)–(1.4) to a p -Laplacian boundary value problem where the differential operator has trivial solutions

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Summary

Introduction

Abstract: In this work, we apply Leray-Schauder continuation principle to establish the existence of at least one solution to the third order p-Laplacian boundary value problem on an unbounded domain of the form (w(t)φp(u′′(t)))′ = K(t, u(t), u′(t), u′′(t)), t ∈ (0, ∞) The purpose of this paper is to obtain existence of at least one solution for the third order p-Laplacian boundary value problem (w(t)φp(u′′(t)))′ = K(t, u(t), u′(t), u′′(t)), t ∈ (0, ∞) In [6] we proved the existence of solutions for the boundary value problem.

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