2002
DOI: 10.1002/nme.443
|View full text |Cite
|
Sign up to set email alerts
|

An improved unsteady, unstructured, artificial compressibility, finite volume scheme for viscous incompressible flows: Part II. Application

Abstract: SUMMARYIn Part I of this paper, a preconditioned artiÿcial compressibility scheme was developed for modelling laminar steady-state and transient, incompressible ows for a wide range of Reynolds and Rayleigh numbers. In this part, several examples of laminar incompressible problems are solved and discussed. The in uence of various AC parameters on robustness and convergence rates are assessed for a complex category of problems. It is shown that the scheme developed in Part I is an accurate, robust and easy to u… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

7
43
0

Year Published

2007
2007
2017
2017

Publication Types

Select...
7

Relationship

3
4

Authors

Journals

citations
Cited by 53 publications
(50 citation statements)
references
References 18 publications
7
43
0
Order By: Relevance
“…They applied the method for problems including lid-driven cavity, backward facing step, buoyancy-driven cavity flow, and Von Karmann vortex street [48]. Nevertheless, the numerical experimentation performed in this study showed that by employing the MPM in the viscous flows over the NACA-hydrofoils, the convergence occurs at low level convergence criteria.…”
Section: Power-law Preconditionermentioning
confidence: 80%
See 1 more Smart Citation
“…They applied the method for problems including lid-driven cavity, backward facing step, buoyancy-driven cavity flow, and Von Karmann vortex street [48]. Nevertheless, the numerical experimentation performed in this study showed that by employing the MPM in the viscous flows over the NACA-hydrofoils, the convergence occurs at low level convergence criteria.…”
Section: Power-law Preconditionermentioning
confidence: 80%
“…Actually, the introduced preconditioning scheme is the extended and modified one which was originally initiated by Malan [2] (Malan's PM). It is worth to mention that Malan applied his method for problems including lid-driven cavity, backward facing step, buoyancy-driven cavity flow, and Von Karmann vortex street [48].…”
Section: Introductionmentioning
confidence: 99%
“…where u i are the Cartesian components of the velocity vector, is the fluid density, p represents the pressure and is an artificial compressibility parameter [36][37][38][39][40][41][42][43][44]. The deviatoric stress components ij are related to the velocity gradients by…”
Section: The Navier-stokes Equations For Incompressible Flowmentioning
confidence: 99%
“…The system of equations is made up of the momentum equations and the incompressibility relation, and it is well known that the main difficulties in its solution reside in the approximation of the convective term and in the calculation of the pressure. A large amount of numerical methods have been developed particularly in the framework of finite elements (FE) (Baker, Dougalis, & Karakashian, 1982;Choi, Choi, & Yoo, 1997;Codina & Soto, 2004;Plana Fattori, Chantoiseau, Doursat, & Flick, 2013;Sun, Zhang, & Ren, 2012), of cell-centred finite volumes (Deponti, Pennati, & De Biase, 2006;Feraudi & Pennati, 1997;Kim & Moin, 1985;Pai, Prakash, & Patnaik, 2013) or cell-vertex finite volumes (Hookey & Baliga, 1998;Malan, Lewis, & Nithiarasu, 2002;Tritthart & Gutknecht, 2007;Vrahliotis, Pappou, & Tsangaris, 2012) and finite differences (Ali, Fieldhouse, & Talbot, 2011;Kumar, Dass, & Dewan, 2010;Shih & Tan, 1989). In the finite difference (FD) and finite volume (FV) *Corresponding author.…”
Section: Introductionmentioning
confidence: 99%