弹性基础上有限梁挠曲定常边值问题的一类积分算子的谱分析:特征方程

S. Choi
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引用次数: 2

摘要

考虑弹性地基上有限梁在竖向荷载作用下挠度的边值问题。我们构造了一个等价的适定两点边界条件集到$\mathrm{gl}(4,\mathbb{C})$的一一对应$\Gamma$。利用$\Gamma$,我们为每个由$\mathbf{M} \in \mathrm{gl}(4,8,\mathbb{C})$表示的适定两点边界条件导出了积分算子$\mathcal{K}_\mathbf{M}$的特征条件。本征条件的特殊特征包括;(1)分离了边界条件$\mathbf{M}$对$\mathrm{Spec}\,\mathcal{K}_\mathbf{M}$的影响;(2)将结构已知的$\mathrm{Spec}\,\mathcal{K}_\mathbf{M}$与$\mathrm{Spec}\,\mathcal{K}_{l,\alpha,k}$连接起来。利用本征条件,我们证明了,对于每一个非零实数$\lambda \not \in \mathrm{Spec}\,\mathcal{K}_{l,\alpha,k}$,存在一个实的适定边界条件$\mathbf{M}$,使得$\lambda \in \mathrm{Spec}\,\mathcal{K}_\mathbf{M}$。这特别表明,由适定边界条件产生的积分算子$\mathcal{K}_\mathbf{M}$通常可能不是正的,也不是收缩的,这与$\mathcal{K}_{l,\alpha,k}$相反。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Spectral analysis for the class of integral operators arising from well-posed boundary value problems of finite beam deflection on elastic foundation: characteristic equation
We consider the boundary value problem for the deflection of a finite beam on an elastic foundation subject to vertical loading. We construct a one-to-one correspondence $\Gamma$ from the set of equivalent well-posed two-point boundary conditions to $\mathrm{gl}(4,\mathbb{C})$. Using $\Gamma$, we derive eigenconditions for the integral operator $\mathcal{K}_\mathbf{M}$ for each well-posed two-point boundary condition represented by $\mathbf{M} \in \mathrm{gl}(4,8,\mathbb{C})$. Special features of our eigenconditions include; (1) they isolate the effect of the boundary condition $\mathbf{M}$ on $\mathrm{Spec}\,\mathcal{K}_\mathbf{M}$, (2) they connect $\mathrm{Spec}\,\mathcal{K}_\mathbf{M}$ to $\mathrm{Spec}\,\mathcal{K}_{l,\alpha,k}$ whose structure has been well understood. Using our eigenconditions, we show that, for each nonzero real $\lambda \not \in \mathrm{Spec}\,\mathcal{K}_{l,\alpha,k}$, there exists a real well-posed boundary condition $\mathbf{M}$ such that $\lambda \in \mathrm{Spec}\,\mathcal{K}_\mathbf{M}$. This in particular shows that the integral operators $\mathcal{K}_\mathbf{M}$ arising from well-posed boundary conditions, may not be positive nor contractive in general, as opposed to $\mathcal{K}_{l,\alpha,k}$.
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