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Finite difference approach to fourth-order linear boundary-value problems
arXiv - CS - Numerical Analysis Pub Date : 2020-04-03 , DOI: arxiv-2004.01433 Matania Ben-Artzi, Benjamin Kramer
arXiv - CS - Numerical Analysis Pub Date : 2020-04-03 , DOI: arxiv-2004.01433 Matania Ben-Artzi, Benjamin Kramer
Discrete approximations to the equation \begin{equation*} L_{cont}u = u^{(4)} + D(x) u^{(3)} + A(x) u^{(2)} +
(A'(x)+H(x)) u^{(1)} + B(x) u = f, \; x\in[0,1] \end{equation*} are considered.
This is an extension of the Sturm-Liouville case $D(x)\equiv H(x)\equiv 0$ [ M.
Ben-Artzi, J.-P. Croisille, D. Fishelov and R. Katzir, Discrete fourth-order
Sturm-Liouville problems, IMA J. Numer. Anal. {\bf 38} (2018), 1485-1522. doi:
10.1093/imanum/drx038] to the non-self-adjoint setting. The "natural" boundary
conditions in the Sturm-Liouville case are the values of the function and its
derivative. The inclusion of a third-order discrete derivative entails a
revision of the underlying discrete functional calculus. This revision forces
evaluations of accurate discrete approximations to the boundary values of the
second, third and fourth order derivatives. The resulting functional calculus
provides the discrete analogs of the fundamental Sobolev
properties--compactness and coercivity. It allows to obtain a general
convergence theorem of the discrete approximations to the exact solution. Some
representative numerical examples are presented.
中文翻译:
四阶线性边值问题的有限差分法
方程的离散近似值 \begin{equation*} L_{cont}u = u^{(4)} + D(x) u^{(3)} + A(x) u^{(2)} + ( A'(x)+H(x)) u^{(1)} + B(x) u = f, \; x\in[0,1] \end{equation*} 被考虑。这是 Sturm-Liouville 案例 $D(x)\equiv H(x)\equiv 0$ [M. Ben-Artzi, J.-P. Croisille、D. Fishelov 和 R. Katzir,离散四阶 Sturm-Liouville 问题,IMA J. Numer。肛门。{\bf 38} (2018),1485-1522。doi: 10.1093/imanum/drx038] 到非自伴随设置。Sturm-Liouville 案例中的“自然”边界条件是函数及其导数的值。包含三阶离散导数需要对基础离散泛函演算进行修订。此修订版强制评估第二个边界值的精确离散近似值,三阶和四阶导数。由此产生的函数演算提供了基本 Sobolev 属性的离散模拟——紧凑性和矫顽力。它允许获得精确解的离散近似的一般收敛定理。给出了一些有代表性的数值例子。
更新日期:2020-04-06
中文翻译:
四阶线性边值问题的有限差分法
方程的离散近似值 \begin{equation*} L_{cont}u = u^{(4)} + D(x) u^{(3)} + A(x) u^{(2)} + ( A'(x)+H(x)) u^{(1)} + B(x) u = f, \; x\in[0,1] \end{equation*} 被考虑。这是 Sturm-Liouville 案例 $D(x)\equiv H(x)\equiv 0$ [M. Ben-Artzi, J.-P. Croisille、D. Fishelov 和 R. Katzir,离散四阶 Sturm-Liouville 问题,IMA J. Numer。肛门。{\bf 38} (2018),1485-1522。doi: 10.1093/imanum/drx038] 到非自伴随设置。Sturm-Liouville 案例中的“自然”边界条件是函数及其导数的值。包含三阶离散导数需要对基础离散泛函演算进行修订。此修订版强制评估第二个边界值的精确离散近似值,三阶和四阶导数。由此产生的函数演算提供了基本 Sobolev 属性的离散模拟——紧凑性和矫顽力。它允许获得精确解的离散近似的一般收敛定理。给出了一些有代表性的数值例子。