This paper analyses the accuracy and numerical stability of coupling procedures in aeroelastic modelling. A twodimensional model problem assuming unsteady inviscid flow past an oscillating wall leads to an even simpler one-dimensional model problem. Analysis of different numerical algorithms shows t
Stability and accuracy of optimal local non-reflecting boundary conditions
โ Scribed by Avram Sidi; Dan Givoli
- Publisher
- Elsevier Science
- Year
- 2000
- Tongue
- English
- Weight
- 220 KB
- Volume
- 33
- Category
- Article
- ISSN
- 0168-9274
No coin nor oath required. For personal study only.
โฆ Synopsis
Problems in unbounded domains are often solved numerically by truncating the infinite domain via an artificial boundary B and applying some boundary condition on B, which is called a Non-Reflecting Boundary Condition (NRBC). Recently, a two-parameter hierarchy of optimal local NRBCs of increasing order has been developed. The optimality is in the sense that the local NRBC best approximates the exact nonlocal Dirichlet-to-Neumann (DtN) boundary condition in the L 2 norm for functions in C โ . The optimal NRBCs are combined with finite element discretization in the computational domain. Here the theoretical properties of the resulting class of schemes are examined. In particular, theorems are proved regarding the numerical stability of the schemes and their rates of convergence.
๐ SIMILAR VOLUMES
## Abstract A shallow water model with linear timeโdependent dispersive waves in an unbounded domain is considered. The domain is truncated with artificial boundaries โฌ๏ธ where a sequence of highโorder nonโreflecting boundary conditions (NRBCs) proposed by Higdon are applied. Methods devised by Givo
A modiรฟed version of an exact Non-re ecting Boundary Condition (NRBC) รฟrst derived by Grote and Keller is implemented in a รฟnite element formulation for the scalar wave equation. The NRBC annihilate the รฟrst N wave harmonics on a spherical truncation boundary, and may be viewed as an extension of th
Starting from known functions, u, (x, y) (i = 1-4) we construct a system of non-linear second-order partial differential equations, which contain basic features of equilibrium conductive, non-ideal MHD equations. This system of equations is then used as a test case for the implementation of the code