Artificial Viscosity Models for Vortex and Particle Methods
โ Scribed by G.-H. Cottet
- Publisher
- Elsevier Science
- Year
- 1996
- Tongue
- English
- Weight
- 1000 KB
- Volume
- 127
- Category
- Article
- ISSN
- 0021-9991
No coin nor oath required. For personal study only.
โฆ Synopsis
It turns out that the precise form of the error produced by vortex methods, and not only their order of conver-
The analysis of the truncation error produced by particle methods leads to artificial viscosity schemes. For vortex methods, they can be gence, can be precisely analyzed. This feature, which defiseen as eddy viscosity models, with anisotropic non-linear diffusion nitely distinguishes vortex methods from grid-based methtensors. Numerical experiments on decaying incompressible 2D ods, stems from the fact that vortex methods and, more turbulence illustrate the efficiency of the method, and in particular generally, particle methods are based on exact weak soluthe fact that the diffusion stops acting in large coherent eddies.
tions of advection equations. The truncation error solely
For compressible flows, this approach allows us to understand the oscillations produced by particle methods and to derive new artifi-results from the mollification used in practice in the compucial viscosity schemes.
๐ SIMILAR VOLUMES
A vortex particle method is developed for simulating two-dimensional, unsteady compressible flow. The method uses the Helmholtz decomposition of the velocity field to separately treat the irrotational and solenoidal portions of the flow, and the particles are allowed to change volume to conserve mas
This paper presents a three-dimensional viscous vortex method for the simulation of particulate flows with two-way coupling. The flow is computed using Lagrangian vortex elements advected with the local velocity, while their strength is modified to account for viscous diffusion, vortex stretching, a