Preview

Proceedings of the Institute for System Programming of the RAS (Proceedings of ISP RAS)

Advanced search

The LS-STAG Immersed Boundary Method Modification for Viscoelastic Flow Computations

https://doi.org/10.15514/ISPRAS-2017-29(1)-5

Abstract

The LS-STAG immersed boundary cut-cell method modification for viscoelastic flow computations is presented. Rate type viscoelastic flow models (linear and quasilinear) are considered. Formulae for differential types of convected time derivatives the LS-STAG discretization was obtained. Normal non-newtonian stresses are computed at the centers of base LS-STAG mesh cells and shear non-newtonian stresses are computed at the cell corners. The LS-STAG-discretization of extra-stress equations for viscoelastic Maxwell, Jeffreys, upper-convected Maxwell, Maxwell-A, Oldroyd-B, Oldroyd-A, Johnson - Segalman fluids was developed. Time-stepping algorithm is defined by the following three steps. Firstly, a prediction of the velocity and pressure correction are computed by means of semi-implicit Euler scheme. Secondly, the provisional velocity is corrected to get a solenoidal velocity and the corresponding pressure field. After this the extra-stress equations are solved. Applications to popular benchmarks for viscoelastic flows with stationary boundaries and comparisons with experimental and numerical studies are presented. The results show that the developed LS-STAG method modification demonstrates an accuracy comparable to body-fitted methods. The obtained modification is implemented in the «LS-STAG» software package developed by the author. This software allows to simulate viscous incompressible flows around a moving airfoil of arbitrary shape or airfoils system with one or two degrees of freedom. For example, it allows to simulate rotors autorotation and airfoils system wind resonance. Intel® Cilk™ Plus, Intel® TBB and OpenMP parallel programming technologies are used in the «LS-STAG».

About the Author

V. . Puzikova
BMSTU
Russian Federation


References

1. Owens R.G., Phillips T.N. Computational Rheology. London: Imperial College Press, 2002. 417 p.

2. Galdi G.P., Rannacher R., Robertson A.M., Turek S. Hemodynamical Flows: Modeling, Analysis and Simulation. N. Y.: Springer, 2008. 501 p.

3. Kim J.M., Kim C., Kim J.H., Chung C., Ahn K.H., Lee S.J. High-resolution finite element simulation of 4:1 planar contraction flow of viscoelastic fluid. J. Non-Newtonian Fluid Mech. 2005, no. 129, pp. 23-37.

4. Mittal R., Iaccarino G. Immersed boundary methods. Annu. Rev. Fluid Mech., 2005, no. 37, pp. 239-261.

5. Cheny Y., Botella O. The LS-STAG method: A new immersed boundary/level-set method for the computation of incompressible viscous flows in complex moving geometries with good conservation properties. J.Comp.Phys., 2010, no.229, pp.1043-1076.

6. Osher S., Fedkiw R.P. Level set methods and dynamic implicit surfaces. N. Y.: Springer, 2003. 273 p.

7. Puzikova V.V., Marchevsky I.K. Extension of the LS-STAG immersed boundary method for RANS-based turbulence models and its application for numerical simulation in coupled hydroelastic problems. Proc. VI International Conference on Coupled Problems in Science and Engineering. Venice, 2015, pp. 532-543.

8. Puzikova V.V. On generalization of the LS-STAG immersed boundary method for Large Eddy Simulation and Detached Eddy Simulation. Proc. Advanced Problems in Mechanics International Summer School-Conference. St.-Petersburg. 2015, pp. 411-417.

9. Marchevsky I., Puzikova V. Application of the LS-STAG Immersed Boundary Method for Numerical Simulation in Coupled Aeroelastic Problems. Proc. 11th World Congress on Computational Mechanics, 5th European Conference on Computational Mechanics, 6th European Conference on Computational Fluid Dyn. Barcelona, 2014, pp.1995-2006.

10. Puzikova V.V. Realization of parallel computations in the software package «LS-STAG_turb» for viscous incompressible flow simulation on systems with shared memory. Trudy ISP RAN / Proc. ISP RAS, vol. 28, issue 1, 2016, pp. 221-242 (in Russian). DOI: 10.15514/ISPRAS-2016-28(1)-13.

11. Uilkinson U.L. Non-newtonian fluids. Moscow: Мир, 1964. 216 p. (in Russian)

12. Maxwell J.C. On the dynamical theory of gases. Philos. Trans. R. Soc. 1867, no. 157, P. 49-88.

13. Jeffreys H. The Earth Its Origin, History and Physical Constitution. Cambridge: Cambridge University Press, 1929. 612 p.

14. Oldroyd J.G. On the formulation of rheological equations of state. Proc. Roy. Soc. London. 1950, no. 200, pp. 523-541.

15. Johnson M.W., Segalman D. A model for viscoelastic fluid behavior which allows non-affine deformation. J. Non-Newton. Fluid Mech., 1977, no. 2, pp. 255-270.

16. Intel® Cilk™ Plus. URL: https://software.intel.com/ru-ru/node/522579 (accessed: 25.10.2015).

17. Reinders J. Intel Threading Building Blocks: Outfitting C++ for Multi-Core Processor Parallelism. Sebastopol: O'Reilly, 2007. 336 p.

18. Keiller R.A. Spatial decay of steady perturbations of plane Poiseuille flow for the Oldroyd-B equation. J. Non-Newton. Fluid Mech., 1993, vol. 46, pp. 129-142.

19. Hayat T., Khan M., Ayub M. Exact solutions of flow problems of an Oldroyd-B fluid. · J. Applied Math. and Comp. 2004, vol. 151, pp. 105-119.


Review

For citations:


Puzikova V. The LS-STAG Immersed Boundary Method Modification for Viscoelastic Flow Computations. Proceedings of the Institute for System Programming of the RAS (Proceedings of ISP RAS). 2017;29(1):71-84. (In Russ.) https://doi.org/10.15514/ISPRAS-2017-29(1)-5



Creative Commons License
This work is licensed under a Creative Commons Attribution 4.0 License.


ISSN 2079-8156 (Print)
ISSN 2220-6426 (Online)