A parallel computational implementation of modern meshless methods is presented for explicit dynamic analysis. The procedures are demonstrated by application of the Reproducing Kernel Particle Method (RKPM). Aspects of a coarse grain parallel paradigm are detailed for a Lagrangian formulation using
Topological aspects of meshless methods and nodal ordering for meshless discretizations
β Scribed by Arash Yavari; Ali Kaveh; Shahram Sarkani; Hosein Ali Rahimi Bondarabady
- Publisher
- John Wiley and Sons
- Year
- 2001
- Tongue
- English
- Weight
- 206 KB
- Volume
- 52
- Category
- Article
- ISSN
- 0029-5981
- DOI
- 10.1002/nme.239
No coin nor oath required. For personal study only.
β¦ Synopsis
Abstract
The meshless elementβfree Galerkin method (EFGM) is considered and compared to the finiteβelement method (FEM). In particular, topological aspects of meshless methods as the nodal connectivity and invertibility of matrices are studied and compared to those of the FE method. We define four associated graphs for meshless discretizations of EFGM and investigate their connectivity. The ways that the associated graphs for coupled FEβEFG models might be defined are recommended. The associated graphs are used for nodal ordering of meshless models in order to reduce the bandwidth, profile, maximum frontwidth, and rootβmeanβsquare wavefront of the corresponding matrices. Finally, the associated graphs are numerically compared. Copyright Β© 2001 John Wiley & Sons, Ltd.
π SIMILAR VOLUMES
We describe an approach to construct approximation basis functions for meshless methods, which is based on the concept of a partition of unity. The approach has the following properties: (i) the grid consists of scattered nodes, (ii) the basis reproduces exactly complete linear polynomials, (iii) on
## Abstract A modified version of the equilibrium on line method (ELM) for imposition of Neumann boundary conditions in collocation methods is presented. In the ELM, equilibrium on lines in the local coordinate systems on the Neumann boundary is satisfied as Neumann boundary condition equations. In