English

Constant sign Green's function for simply supported beam equation

Classical Analysis and ODEs 2016-04-18 v2

Abstract

The aim of this paper consists on the study of the following fourth-order operator: \begin{equation}\label{Ec::T4} T[M]\,u(t)\equiv u^{(4)}(t)+p_1(t)\,u"'(t)+p_2(t)\,u"(t)+M\,u(t)\,,\ t\in I \equiv [a,b]\,, \end{equation} coupled with the two point boundary conditions: \begin{equation}\label{Ec::cf} u(a)=u(b)=u"(a)=u"(b)=0\,. \end{equation} So, we define the following space: \begin{equation}\label{Ec::esp} X=\left\lbrace u\in C^4(I)\quad\mid\quad u(a)=u(b)=u"(a)=u"(b)=0 \right\rbrace \,. \end{equation} Here p1C3(I)p_1\in C^3(I) and p2C2(I)p_2\in C^2(I). By assuming that the second order linear differential equation \begin{equation}\label{Ec::2or} L_2\, u(t)\equiv u"(t)+p_1(t)\,u'(t)+p_2(t)\,u(t)=0\,,\quad t\in I, \end{equation} is disconjugate on II, we characterize the parameter's set where the Green's function related to operator T[M]T[M] in XX is of constant sign on I×II \times I. Such characterization is equivalent to the strongly inverse positive (negative) character of operator T[M]T[M] on XX and comes from the first eigenvalues of operator T[0]T[0] on suitable spaces.

Cite

@article{arxiv.1604.04245,
  title  = {Constant sign Green's function for simply supported beam equation},
  author = {Alberto Cabada and Lorena Saavedra},
  journal= {arXiv preprint arXiv:1604.04245},
  year   = {2016}
}

Comments

27 pages, 2 figures

R2 v1 2026-06-22T13:32:43.785Z