Explicit expressions for 3D boundary integrals in potential theory
β Scribed by S. Nintcheu Fata
- Publisher
- John Wiley and Sons
- Year
- 2009
- Tongue
- English
- Weight
- 236 KB
- Volume
- 78
- Category
- Article
- ISSN
- 0029-5981
- DOI
- 10.1002/nme.2472
No coin nor oath required. For personal study only.
β¦ Synopsis
Abstract
On employing isoparametric, piecewise linear shape functions over a flat triangular domain, exact expressions are derived for all surface potentials involved in the numerical solution of threeβdimensional singular and hyperβsingular boundary integral equations of potential theory. These formulae, which are valid for an arbitrary source point in space, are represented as analytic expressions over the edges of the integration triangle. They can be used to solve integral equations defined on polygonal boundaries via the collocation method or may be utilized as analytic expressions for the inner integrals in the Galerkin technique. In addition, the constant element approximation can be directly obtained with no extra effort. Sample problems solved by the collocation boundary element method for the Laplace equation are included to validate the proposed formulae. Published in 2008 by John Wiley & Sons, Ltd.
π SIMILAR VOLUMES
Both the logarithmic and derivative kernel integrations for potential problems, solved with quadratic isoparametric boundary elements, contain quartic functions of the integration parameter. It is shown that such functions can be written as the product of two quadratic functions with real coefficien
The boundary node method (BNM) is developed in this paper for solving potential problems in three dimensions. The BNM represents a coupling between boundary integral equations (BIE) and moving least-squares (MLS) interpolants. The main idea here is to retain the dimensionality advantage of the forme
## Abstract An advanced boundary element method (BEM) for solving twoβ (2D) and threeβdimensional (3D) problems in materials with microstructural effects is presented. The analysis is performed in the context of Mindlin's FormβII gradient elastic theory. The fundamental solution of the equilibrium