Positive solutions for nonlocal fourth-order boundary value problems with all order derivatives
12 pages
English

Découvre YouScribe en t'inscrivant gratuitement

Je m'inscris

Positive solutions for nonlocal fourth-order boundary value problems with all order derivatives

-

Découvre YouScribe en t'inscrivant gratuitement

Je m'inscris
Obtenez un accès à la bibliothèque pour le consulter en ligne
En savoir plus
12 pages
English
Obtenez un accès à la bibliothèque pour le consulter en ligne
En savoir plus

Description

In this article, by the fixed point theorem in a cone and the nonlocal fourth-order BVP's Green function, the existence of at least one positive solution for the nonlocal fourth-order boundary value problem with all order derivatives u ( 4 ) ( t ) + A u ″ ( t ) = λ f ( t , u ( t ) , u ′ ( t ) , u ″ ( t ) , u ‴ ( t ) ) , 0 < t < 1 , u ( 0 ) = u ( 1 ) = .

Sujets

Informations

Publié par
Publié le 01 janvier 2012
Nombre de lectures 7
Langue English

Extrait

Guoet al.Boundary Value Problems2012,2012:29 http://www.boundaryvalueproblems.com/content/2012/1/29
R E S E A R C HOpen Access Positive solutions for nonlocal fourthorder boundary value problems with all order derivatives 1 21* Yanping Guo , Fei Yangand Yongchun Liang
* Correspondence: lycocean@163. com 1 College of Electrical Engineering and Information, Hebei University of Science and Technology, Shijiazhuang 050018, Hebei, P. R. China Full list of author information is available at the end of the article
Abstract In this article, by the fixed point theorem in a cone and the nonlocal fourthorder BVPs Green function, the existence of at least one positive solution for the nonlocal fourthorder boundary value problem with all order derivatives (4)   u(t) +Au(t) =λf(t,u(t),u(t),u(t),u(t)), 0<t<1, 1 u(0) =u(1) =p(s)u(s)ds, 0  1   u(0) =u(1) =q(s)u(s)ds 0 2 is considered, wherefis a nonnegative continuous function,l>0, 0< A <π,p, qÎ L[0, 1],p(s)0,q(s)0. The emphasis here is thatfdepends on all order derivatives. Keywords:fourthorder boundary value problem, fixed point theorem, Greens func tion, positive solution
1 Introduction The deformation of an elastic beam in equilibrium state, whose two ends are simply supported, can be described by a fourthorder ordinary equation boundary value pro blem. Owing to its significance in physics, the existence of positive solutions for the fourthorder boundary value problem has been studied by many authors using non linear alternatives of LeraySchauder, the fixed point index theory, the Krasnoselskiis fixed point theorem and the method of upper and lower solutions, in reference [110]. In recent years, there has been much attention on the question of positive solutions of the fourthorder differential equations with one or two parameters. By the Krasno selskiis fixed point theorem in cone [11], Bai [5] investigated the following fourth order boundary value problem with one parameter (4)  u(t) +βu(t) =λf(t,u(t),u(t)), 0<t<1, 1 u(0) =u(1) =p(s)u(s)ds, 0  1   u(0) =u(1) =q(s)u(s)ds, 0 2 wherel>0, 0<b<π,f: C([0, 1] × [0,) × (, 0], [0,)) is continuous,p, qÎL[0, 1],  1 11 p(s)0,q(s)0,p(s)ds<1,q(s) sinβsds+q(s) sinβ(1s)ds<sinβ. 0 00
© 2012 Guo 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.
  • Univers Univers
  • Ebooks Ebooks
  • Livres audio Livres audio
  • Presse Presse
  • Podcasts Podcasts
  • BD BD
  • Documents Documents