A weighted meshfree collocation method for incompressible flows using radial basis functions
A weighted strong form collocation method using radial basis functions and explicit time integration is proposed to solve the incompressible Navier-Stokes equations. The velocities and pressure are solved directly at the same time step and the continuity equation is satisfied at each time step which...
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| Vydáno v: | Journal of computational physics Ročník 401; s. 108964 |
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| Hlavní autoři: | , , , |
| Médium: | Journal Article |
| Jazyk: | angličtina |
| Vydáno: |
Cambridge
Elsevier Inc
15.01.2020
Elsevier Science Ltd |
| Témata: | |
| ISSN: | 0021-9991, 1090-2716 |
| On-line přístup: | Získat plný text |
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| Shrnutí: | A weighted strong form collocation method using radial basis functions and explicit time integration is proposed to solve the incompressible Navier-Stokes equations. The velocities and pressure are solved directly at the same time step and the continuity equation is satisfied at each time step which improve the solution accuracy and stability. No artificial compressibility coefficient needs to be introduced for modeling the incompressible flows and no pressure oscillation arises in the numerical solutions. Optimal convergence can be achieved by imposing the derived proper weights on the boundaries and the continuity equation. Radial basis collocation method in a Lagrangian form is quite easy to capture the moving boundary or free surface in flow problems. Moreover, solid boundary conditions can be enforced directly and no special treatments are required. Further, critical time step for the explicit time integration is predicted in the stability analysis and the influences on the stability are evaluated. Numerical studies validate the high accuracy as well as good stability of the presented method.
•A weighted collocation method is raised for incompressible Navier-Stokes equations.•Optimal convergence can be gained by imposing the proper weights on the boundaries.•No artificial compressibility coefficient is used to model the incompressible flow.•No pressure oscillation arises in the numerical solutions.•It's quite easy to capture the moving boundary or free surface in flow problems. |
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| Bibliografie: | ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 14 |
| ISSN: | 0021-9991 1090-2716 |
| DOI: | 10.1016/j.jcp.2019.108964 |