Global structure of positive solutions for a fourth-order boundary value problem with singular data

Pub Date : 2023-09-30 DOI:10.4171/zaa/1729
Ruyun Ma, Zhongzi Zhao, Mantang Ma
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Abstract

We are concerned with a problem described the deformation of a simply supported beam of the form $$ u^{(4)}(x)+c(x)u(x) + \sum^p\_{i=1}c\_i\delta(x-x\_i)u(x) = \lambda a(u(x)) + \lambda\sum^q\_{j=1}a\_j(u(x))\delta(x-y\_j), \quad x\in (0,1), $$ $$ u(0)=u(1)=u''(0)=u''(1)=0, $$ where $\lambda$ is a positive parameter, $c\in C(\[0, 1],\mathbb{R})$, $c\_i \in \mathbb{R}$, $a, a\_j\in C(\[0,\infty),\[0,\infty))$, $i = 1, 2, \ldots, p$, $j= 1, 2, \ldots, q$, $p, q \in \mathbb{N}$. The Dirac delta impulses $\delta = \delta(x)$ are applied at given points $0 < x\_1 < x\_2 <\cdots < x\_p < 1$ and $0 < y\_1 < y\_2 < \cdots < y\_q < 1$. We investigate the global structure of positive solutions by the global bifurcation techniques.
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一类具有奇异数据的四阶边值问题正解的全局结构
我们关注的是形式为$$ u^{(4)}(x)+c(x)u(x) + \sum^p\_{i=1}c\_i\delta(x-x\_i)u(x) = \lambda a(u(x)) + \lambda\sum^q\_{j=1}a\_j(u(x))\delta(x-y\_j), \quad x\in (0,1), $$$$ u(0)=u(1)=u''(0)=u''(1)=0, $$的简支梁的变形问题,其中$\lambda$是一个正参数,$c\in C(\[0, 1],\mathbb{R})$, $c\_i \in \mathbb{R}$, $a, a\_j\in C(\[0,\infty),\[0,\infty))$, $i = 1, 2, \ldots, p$, $j= 1, 2, \ldots, q$, $p, q \in \mathbb{N}$。狄拉克脉冲$\delta = \delta(x)$应用于给定点$0 < x\_1 < x\_2 <\cdots < x\_p < 1$和$0 < y\_1 < y\_2 < \cdots < y\_q < 1$。利用全局分岔技术研究了正解的全局结构。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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