We propose and analyze a finite element method for approximating solutions to the Navier-Stokes-alpha model (NS-α) that utilizes approximate deconvolution and a modified grad-div stabilization and greatly improves accuracy in simulations. Standard finite element schemes for NS-α suffer from two major sources of error if their solutions are considered approximations to true fluid flow: (1) the consistency error arising from filtering; and (2) the dramatic effect of the large pressure error on the velocity error that arises from the (necessary) use of the rotational form nonlinearity. The proposed scheme “fixes” these two numerical issues through the combined use of a modified grad-div stabilization that acts in both the momentum and filter equations, and an adapted approximate deconvolution technique designed to work with the altered filter. We prove the scheme is stable, optimally convergent, and the effect of the pressure error on the velocity error is significantly reduced. Several numerical experiments are given that demonstrate the effectiveness of the method.
@article{M2AN_2011__45_2_277_0, author = {Manica, Carolina C. and Neda, Monika and Olshanskii, Maxim and Rebholz, Leo G.}, title = {Enabling numerical accuracy of Navier-Stokes-$\alpha $ through deconvolution and enhanced stability}, journal = {ESAIM: Mathematical Modelling and Numerical Analysis - Mod\'elisation Math\'ematique et Analyse Num\'erique}, volume = {45}, year = {2011}, pages = {277-307}, doi = {10.1051/m2an/2010042}, zbl = {1267.76021}, language = {en}, url = {http://dml.mathdoc.fr/item/M2AN_2011__45_2_277_0} }
Manica, Carolina C.; Neda, Monika; Olshanskii, Maxim; Rebholz, Leo G. Enabling numerical accuracy of Navier-Stokes-$\alpha $ through deconvolution and enhanced stability. ESAIM: Mathematical Modelling and Numerical Analysis - Modélisation Mathématique et Analyse Numérique, Tome 45 (2011) pp. 277-307. doi : 10.1051/m2an/2010042. http://gdmltest.u-ga.fr/item/M2AN_2011__45_2_277_0/
[1] On the approximate deconvolution procedure for LES. Phys. Fluids 2 (1999) 1699-1701. | Zbl 1147.76506
and ,[2] Deconvolution methods for subgrid-scale approximation in large eddy simulation, Modern Simulation Strategies for Turbulent Flow. R.T. Edwards (2001).
and ,[3] Galerkin approximations for the Navier-Stokes equations. Harvard University (1976).
,[4] Improved subgrid scale models for large eddy simulation. AIAA Pap. (1983).
, and ,[5] Mathematics of Large Eddy Simulation of Turbulent Flows, Scientific Computation. Springer (2006). | MR 2185509 | Zbl 1089.76002
, and ,[6] The Mathematical Theory of Finite Element Methods. Springer-Verlag (1994). | MR 1278258 | Zbl 1012.65115
and ,[7] Pressure projection stabilizations for Galerkin approximations of Stokes' and Darcy's problem. Numer. Methods Partial Differ. Equ. 24 (2008) 127-143. | MR 2371351 | Zbl 1139.76029
,[8] Stabilized finite element schemes for incompressible flow using Scott-Vogelius elements. Appl. Num. Math. 58 (2008) 1704-1719. | MR 2458477 | Zbl 1148.76031
and ,[9] An integrable shallow water equation with peaked solutions. Phys. Rev. Lett. 71 (1993) 1661-1664. | MR 1234453 | Zbl 0972.35521
and ,[10] The Camassa-Holm equations as a closure model for turbulent channel and pipe flow. Phys. Rev. Lett. 81 (1998) 5338-5341. | MR 1745983 | Zbl 1042.76525
, , , , and ,[11] The Camassa-Holm equations and turbulence. Physica D 133 (1999) 49-65. | MR 1721139 | Zbl 1194.76069
, , , , and ,[12] Direct numerical simulations of the Navier-Stokes alpha model. Physica D 133 (1999) 66-83. | MR 1721140 | Zbl 1194.76080
, , and ,[13] Numerical solution for the Navier-Stokes equations. Math. Comp. 22 (1968) 745-762. | MR 242392 | Zbl 0198.50103
,[14] A locally conservative LDG method for the incompressible Navier-Stokes equations. Math. Comp. 74 (2005) 1067-1095. | MR 2136994 | Zbl 1069.76029
, and ,[15] Stabilized finite element approximation of transient incompressible flows using orthogonal subscales. Comput. Methods Appl. Mech. Engrg. 191 (2002) 4295-4321. | MR 1925888 | Zbl 1015.76045
,[16] Convergence analysis and computational testing of the finite element discretization of the Navier-Stokes-alpha model. Numer. Methods Partial Differ. Equ. (to appear). | MR 2732382 | Zbl pre05814514
,[17] Exact fully 3d Navier-Stokes solutions for benchmarking. Int. J. Numer. Methods Fluids 19 (1994) 369-375. | Zbl 0814.76031
and ,[18] Stabilized finite element methods. II. The incompressible Navier-Stokes equations. Comput. Methods Appl. Mech. Engrg. 99 (1992) 209-233. | MR 1186727 | Zbl 0765.76048
and ,[19] The Navier-Stokes-alpha model of fluid turbulence. Physica D 152-153 (2001) 505-519. | MR 1837927 | Zbl 1037.76022
, and ,[20] The three dimensional viscous Camassa-Holm equations, and their relation to the Navier-Stokes equations and turbulence theory. J. Dyn. Diff. Equ. 14 (2002) 1-35. | MR 1878243 | Zbl 0995.35051
, and ,[21] Stabilized finite element schemes with LBB-stable elements for incompressible flows. J. Comput. Appl. Math. 177 (2005) 243-267. | MR 2125317 | Zbl 1063.76054
, , and ,[22] Large eddy simulation of turbulent incompressible flows by a three-level finite element method. Int. J. Numer. Methods Fluids 48 (2005) 1067-1099. | MR 2152771 | Zbl 1070.76034
, and ,[23] Mechanism of the production of small eddies from larger ones. Proc. Royal Soc. A 158 (1937) 499-521. | JFM 63.1358.03
and ,[24] An interpretation of the Navier-Stokes-alpha model as a frame-indifferent Leray regularization. Physica D 177 (2003) 23-30. | MR 1965324 | Zbl 1082.35120
, and ,[25] Finite Element Methods for Viscous Incompressible Flow: A Guide to Theory, Practice, and Algorithms. Academic Press, Boston (1989). | MR 1017032 | Zbl 0697.76031
,[26] A velocity-pressure streamline diffusion method for the incompressible Navier-Stokes equations. Comput. Methods Appl. Mech. Engrg. 84 (1990) 175-192. | MR 1087615 | Zbl 0716.76048
and ,[27] Numerical studies of finite element variational multiscale methods for turbulent flow simulations. Comput. Methods Appl. Mech. Engrg. 199 (2010) 841-852. | MR 2581347 | Zbl pre05685178
and ,[28] Analysis of numerical errors in Large Eddy Simulation. SIAM J. Numer. Anal. 40 (2002) 995-1020. | MR 1949402 | Zbl 1026.76028
and ,[29] Time dependent flow across a step: the slip with friction boundary condition. Int. J. Numer. Methods Fluids 50 (2006) 713-731. | MR 2199095 | Zbl 1086.76040
and ,[30] A remark on regularity of an elliptic-elliptic singular perturbation problem. Technical report, University of Pittsburgh (2007).
,[31] Introduction to the numerical analysis of incompressible viscous flows. SIAM (2008). | MR 2442411 | Zbl 1153.76002
,[32] Numerical analysis and computational testing of a high-accuracy Leray-deconvolution model of turbulence. Numer. Methods Partial Differ. Equ. 24 (2008) 555-582. | MR 2382797 | Zbl 1191.76061
, , and ,[33] On the accuracy of the rotation form in simulations of the Navier-Stokes equations. J. Comput. Phys. 228 (2009) 3433-3447. | MR 2513841 | Zbl 1161.76030
, , , and ,[34] Numerical analysis and computational comparisons of the NS-omega and NS-alpha regularizations. Comput. Methods Appl. Mech. Engrg. 199 (2010) 916-931. | MR 2581353 | Zbl pre05685184
, , and ,[35] Energy and helicity dissipation rates of the NS-alpha and NS-alpha-deconvolution models. IMA J. Appl. Math. 75 (2010) 56-74. | MR 2587566 | Zbl pre05681027
, and ,[36] A study of the Navier-Stokes-alpha model for two-dimensional turbulence. J. Turbulence 8 (2007) 751-778. | MR 2392989 | Zbl 1039.35078
, , and ,[37] Global well-posedness for the lagrangian averaged Navier-Stokes (lans-alpha) equations on bounded domains. Philos. Trans. Roy. Soc. London A 359 (2001) 14-49. | MR 1853633 | Zbl 1006.35074
and ,[38] Some remarks on residual-based stabilisation of inf-sup stable discretisations of the generalised Oseen problem. Comput. Meth. Appl. Math. 198 (2009) 368-390. | MR 2641303 | Zbl 1245.76051
, and ,[39] Computing NS-alpha with greater physical accuracy and higher convergence rates. Numer. Methods Partial Differ. Equ. (to appear).
and ,[40] Helicity in laminar and turbulent flow. Ann. Rev. Fluid Mech. 24 (1992) 281-312. | MR 1145012 | Zbl 0751.76018
and ,[41] A similarity theory of locally homogeneous and isotropic turbulence generated by a Smagorinsky-type LES. J. Fluid Mech. 325 (1996) 239-260. | Zbl 0891.76045
,[42] A low order Galerkin finite element method for the Navier-Stokes equations of steady incompressible flow: a stabilization issue and iterative methods. Comp. Meth. Appl. Mech. Eng. 191 (2002) 5515-5536. | MR 1941488 | Zbl 1083.76553
,[43] Grad-Div stabilization for the Stokes equations. Math. Comput. 73 (2004) 1699-1718. | MR 2059732 | Zbl 1051.65103
and ,[44] Grad-div stabilization and subgrid pressure models for the incompressible Navier-Stokes equations. Comput. Methods Appl. Mech. Engrg. 198 (2009) 3975-3988. | MR 2557485 | Zbl 1231.76161
, , and ,[45] Conservation laws of turbulence models. J. Math. Anal. Appl. 326 (2007) 33-45. | MR 2277764 | Zbl 1110.76028
,[46] A family of new high order NS-alpha models arising from helicity correction in Leray turbulence models. J. Math. Anal. Appl. 342 (2008) 246-254. | MR 2440794 | Zbl 1138.35078
,[47] On the high accuracy NS--deconvolution model of turbulence. Math. Models Methods Appl. Sci. 20 (2010) 611-633. | MR 2647034 | Zbl 1187.76720
and ,[48] Norm estimates for a maximum right inverse of the divergence operator in spaces of piecewise polynomials. RAIRO Modél. Math. Anal. Numér. 19 (1985) 111-143. | Numdam | MR 813691 | Zbl 0608.65013
and ,[49] An approximate deconvolution model for large-eddy simulation with application to incompressible wall-bounded flows. Phys. Fluids 13 (2001) 997. | Zbl 1184.76530
, and ,[50] Application of finite element method in aeroelasticity. J. Comput. Appl. Math. 215 (2008) 586-594. | MR 2406660 | Zbl 1134.76031
,[51] Comparison of some upwind-biased high-order formulations with a second order central-difference scheme for time integration of the incompressible Navier-Stokes equations. Comput. Fluids 25 (1996) 647-665. | MR 1416431 | Zbl 0888.76061
,[52] On decay of vortices in a viscous fluid. Phil. Mag. 46 (1923) 671-674. | JFM 49.0607.02
,