In this paper we present a comparative study of three non-linear schemes for solving ®nite element systems of Navier±Stokes incompressible ¯ows. The ®rst scheme is the classical Newton±Raphson linearization, the second one is the modi®ed Newton±Raphson linearization and the last one is a new scheme
Efficient solving method for unsteady incompressible interfacial flow problems
✍ Scribed by Stéphane Vincent; Jean-Paul Caltagirone
- Publisher
- John Wiley and Sons
- Year
- 1999
- Tongue
- English
- Weight
- 208 KB
- Volume
- 30
- Category
- Article
- ISSN
- 0271-2091
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✦ Synopsis
Unsteady interfacial problems, considered in an Eulerian form, are studied. The phenomena are modeled using the incompressible viscous Navier-Stokes equations to get the velocity field and an advection equation to predict interface evolutions. The momentum equation is solved by means of an implicit hybrid augmented Lagrangian-Projection method, whereas an explicit characteristic method coupled with a TVD SUPERBEE scheme is applied to the advection equation. The velocity components and the pressure are discretized on staggered grids with finite volumes. Emphasis is on the accuracy and robustness of the techniques described before. A precise explanation on the validation phase will be given, which uses such tests as the advection of a step function or Zalesak's problem to improve the calculation of the interface. The global approach is used on a physically hard interfacial test with strong disparities between viscosities and densities.
📜 SIMILAR VOLUMES
A method for computing unsteady incompressible viscous ows on moving or deforming meshes is described. It uses a well-established time-marching ÿnite-volume ow solver, developed for steady compressible ows past rigid bodies. Time-marching methods cannot be applied directly to incompressible ows beca
## Abstract A new meshless local Petrov–Galerkin (MLPG) method, based on local boundary integral equation (LBIE) considerations, is proposed here for the solution of 2D, incompressible and nearly incompressible elastostatic problems. The method utilizes, for its meshless implementation, nodal point