Abstract
Inf-sup stable FEM applied to time-dependent incompressible Navier–Stokes flows are considered. The focus lies on robust estimates for the kinetic and dissipation energies in a twofold sense. Firstly, pressure–robustness ensures the fulfilment of a fundamental invariance principle and velocity error estimates are not corrupted by the pressure approximability. Secondly, Re-semi-robustness means that constants appearing on the right-hand side of kinetic and dissipation energy error estimates (including Gronwall constants) do not explicitly depend on the Reynolds number. Such estimates rely on the essential regularity assumption \(\nabla u \in L^1(0,T;L^\infty (\varOmega ))\) which is discussed in detail. In the sense of best practice, we review and establish pressure- and Re-semi-robust estimates for pointwise divergence-free \(H^1\)-conforming FEM (like Scott–Vogelius pairs or certain isogeometric based FEM) and pointwise divergence-free H(div)-conforming discontinuous Galerkin FEM. For convection-dominated problems, the latter naturally includes an upwind stabilisation for the velocity which is not gradient-based.
Similar content being viewed by others
References
Ahmed, N., Linke, A., Merdon, C.: Towards pressure–robust mixed methods for the incompressible Navier–Stokes equations. Comput. Methods Appl. Math. (2017). https://doi.org/10.1515/cmam-2017-0047
Arndt, D., Braack, M., Lube, G.: Finite elements for the Navier–Stokes problem with outflow condition. In: Karasözen, B., Manguoğlu, M., Tezer-Sezgin, M., Göktepe, S., Uğur, Ö. (eds.) Numerical Mathematics and Advanced Applications ENUMATH 2015. Lecture Notes in Computational Science and Engineering, vol. 112, pp. 95–103. Springer, Cham (2016)
Arndt, D., Dallmann, H., Lube, G.: Local projection FEM stabilization for the time-dependent incompressible Navier–Stokes problem. Numer. Methods Part. Differ. Equ. 31(4), 1224–1250 (2015)
Ascher, U., Ruuth, S., Wetton, B.: Implicit–explicit methods for time-dependent partial differential equations. SIAM J. Numer. Anal. 32(3), 797–823 (1995)
Bardos, C.W., Titi, E.S.: Mathematics and turbulence: where do we stand? J. Turbul. 14(3), 42–76 (2013)
Berselli, L.C., Iliescu, T., Layton, W.J.: Mathematics of Large Eddy Simulation of Turbulent Flows. Springer, Berlin (2006)
Bertoglio, C., Caiazzo, A., Bazilevs, Y., Braack, M., Esmaily, M., Gravemeier, V., Marsden, A., Pironneau, O., Vignon-Clementel, I.E., Wall, W.A.: Benchmark problems for numerical treatment of backflow at open boundaries. Int. J. Numer. Meth. Biomed. Eng. 34(2), e2918 (2018)
Bertozzi, A.L.: Heteroclinic orbits and chaotic dynamics in planar fluid flows. SIAM J. Math. Anal. 19(6), 1271–1294 (1988)
Boffi, D., Brezzi, F., Fortin, M.: Mixed Finite Element Methods and Applications. Springer, Berlin (2013)
Boyer, F., Fabrie, P.: Mathematical Tools for the Study of the Incompressible Navier–Stokes Equations and Related Models. Springer, New York (2013)
Buffa, A., de Falco, C., Sangalli, G.: IsoGeometric analysis: stable elements for the 2D Stokes equation. Int. J. Numer. Methods Fluids 65(11–12), 1407–1422 (2011)
Burman, E.: Robust error estimates for stabilized finite element approximations of the two dimensional Navier–Stokes equations at high Reynolds number. Comput. Methods Appl. Mech. Eng. 288, 2–23 (2015)
Burman, E., Fernández, M.A.: Continuous interior penalty finite element method for the time-dependent Navier–Stokes equations: space discretization and convergence. Numer. Math. 107(1), 39–77 (2007)
Case, M.A., Ervin, V.J., Linke, A., Rebholz, L.G.: A connection between Scott–Vogelius and grad-div stabilized Taylor–Hood FE approximations of the Navier–Stokes equations. SIAM J. Numer. Anal. 49(4), 1461–1481 (2011)
Chacón Rebollo, T., Lewandowski, R.: Mathematical and Numerical Foundations of Turbulence Models and Applications. Birkhäuser Basel, New York (2014)
Chrysafinos, K., Hou, L.S.: Analysis and approximations of the evolutionary Stokes equations with inhomogeneous boundary and divergence data using a parabolic saddle point formulation. ESAIM: M2AN 51(4), 1501–1526 (2017)
Cockburn, B.: Two new techniques for generating exactly incompressible approximate velocities. Comput Fluid Dyn 2006, 1–11 (2009)
Cockburn, B.: Static condensation, hybridization, and the devising of the HDG methods. In: Building Bridges: Connections and Challenges in Modern Approaches to Numerical Partial Differential Equations, pp. 129–177. Springer, New York (2016)
Cockburn, B., Gopalakrishnan, J.: Incompressible finite elements via hybridization. Part I: the Stokes system in two space dimensions. SIAM J. Numer. Anal. 43(4), 1627–1650 (2005)
Cockburn, B., Gopalakrishnan, J.: Incompressible finite elements via hybridization. Part II: the Stokes system in three space dimensions. SIAM J. Numer. Anal. 43(4), 1651–1672 (2005)
Cockburn, B., Gopalakrishnan, J.: The derivation of hybridizable discontinuous Galerkin methods for Stokes flow. SIAM J. Numer. Anal. 47(2), 1092–1125 (2009)
Cockburn, B., Gopalakrishnan, J., Lazarov, R.: Unified hybridization of discontinuous Galerkin, mixed, and continuous Galerkin methods for second order elliptic problems. SIAM J. Numer. Anal. 47(2), 1319–1365 (2009)
Cockburn, B., Kanschat, G., Schötzau, D.: A note on discontinuous Galerkin divergence-free solutions of the Navier–Stokes equations. J. Sci. Comput. 31(1–2), 61–73 (2007)
Cousins, B.R., Le Borne, S., Linke, A., Rebholz, L.G., Wang, Z.: Efficient linear solvers for incompressible flow simulations using Scott–Vogelius finite elements. Numer. Methods Part. Differ. Equ. 29(4), 1217–1237 (2013)
Dallmann, H., Arndt, D.: Stabilized finite element methods for the Oberbeck–Boussinesq model. J. Sci. Comput. 69(1), 244–273 (2016)
Di Pietro, D.A., Ern, A.: Mathematical Aspects of Discontinuous Galerkin Methods. Springer, Berlin (2012)
Durst, F.: Fluid Mechanics: An Introduction to the Theory of Fluid Flows. Springer, Berlin (2008)
Ern, A., Guermond, J.L.: Theory and Practice of Finite Elements. Springer, New York (2004)
Evans, J.A.: Divergence-free B-spline discretizations for viscous incompressible flows. Ph.D. thesis, The University of Texas at Austin (2011)
Evans, J.A., Hughes, T.J.R.: Isogeometric divergence-conforming B-splines for the steady Navier–Stokes equations. Math. Model Methods Appl. Sci. 23(8), 1421–1478 (2013)
Evans, J.A., Hughes, T.J.R.: Isogeometric divergence-conforming B-splines for the unsteady Navier–Stokes equations. J. Comput. Phys. 241, 141–167 (2013)
de Frutos, J., García-Archilla, B., John, V., Novo, J.: Semi-robust local projection stabilization for non inf-sup stable discretizations of the evolutionary Navier–Stokes equations. arXiv:1709.01011 [math.NA] (2017)
de Frutos, J., García-Archilla, B., John, V., Novo, J.: Analysis of the grad-div stabilization for the time-dependent Navier–Stokes equations with inf-sup stable finite elements. Adv. Comput. Math. 44(1), 195–225 (2018)
Girault, V., Nochetto, R.H., Scott, L.R.: Max-norm estimates for Stokes and Navier–Stokes approximations in convex polyhedra. Numer. Math. 131(4), 771–822 (2015)
Guzmán, J., Shu, C.W., Sequeira, F.A.: H(div) conforming and DG methods for incompressible Euler’s equations. IMA J. Numer. Anal. 37(4), 1733–1771 (2017)
Henshaw, W.D., Kreiss, H.O., Reyna, L.G.: Smallest scale estimates for the Navier–Stokes equations for incompressible fluids. Arch. Ration. Mech. Anal. 112(1), 21–44 (1990)
Hesthaven, J.S., Warburton, T.: Nodal Discontinuous Galerkin Methods: Algorithms, Analysis, and Applications. Springer, New York (2007)
Jenkins, E.W., John, V., Linke, A., Rebholz, L.G.: On the parameter choice in grad-div stabilization for the Stokes equations. Adv. Comput. Math. 40(2), 491–516 (2014)
John, V.: Finite Element Methods for Incompressible Flow Problems. Springer, New York (2016)
John, V., Knobloch, P., Novo, J.: Finite elements for scalar convection-dominated equations and incompressible flow problems: a never ending story? Comput. Vis. Sci. (2018). https://doi.org/10.1007/s00791-018-0290-5
John, V., Linke, A., Merdon, C., Neilan, M., Rebholz, L.G.: On the divergence constraint in mixed finite element methods for incompressible flows. SIAM Rev. 59(3), 492–544 (2017)
Lederer, P.L., Lehrenfeld, C., Schöberl, J.: Hybrid discontinuous Galerkin methods with relaxed H(div)-conformity for incompressible flows. Part I. (2017). arXiv:1707.02782 [math.NA]
Lederer, P.L., Linke, A., Merdon, C., Schöberl, J.: Divergence-free reconstruction operators for pressure–robust Stokes discretizations with continuous pressure finite elements. SIAM J. Numer. Anal. 55(3), 1291–1314 (2017)
Lederer, P.L., Schöberl, J.: Polynomial robust stability analysis for \(H(\operatorname{div})\)-conforming finite elements for the Stokes equations. IMA J. Numer. Anal. (2017). https://doi.org/10.1093/imanum/drx051
Lehrenfeld, C.: Hybrid discontinuous Galerkin methods for solving incompressible flow problems. Master’s thesis, RWTH Aachen (2010)
Lehrenfeld, C., Schöberl, J.: High order exactly divergence-free hybrid discontinuous Galerkin methods for unsteady incompressible flows. Comput. Methods Appl. Mech. Eng. 307, 339–361 (2016)
Linke, A.: On the role of the Helmholtz decomposition in mixed methods for incompressible flows and a new variational crime. Comput. Methods Appl. Mech. Eng. 268, 782–800 (2014)
Linke, A., Matthies, G., Tobiska, L.: Robust arbitrary order mixed finite element methods for the incompressible Stokes equations with pressure independent velocity errors. ESAIM: M2AN 50(1), 289–309 (2016)
Linke, A., Merdon, C.: On velocity errors due to irrotational forces in the Navier–Stokes momentum balance. J. Comput. Phys. 313, 654–661 (2016)
Linke, A., Merdon, C.: Pressure–robustness and discrete Helmholtz projectors in mixed finite element methods for the incompressible Navier-Stokes equations. Comput. Methods Appl. Mech. Eng. 311, 304–326 (2016)
Lube, G., Arndt, D., Dallmann, H.: Understanding the limits of inf-sup stable Galerkin-FEM for incompressible flows. In: Knobloch, P. (ed.) Boundary and Interior Layers, Computational and Asymptotic Methods—BAIL 2014. Lecture Notes in Computational Science and Engineering, vol. 108, pp. 147–169. Springer, Cham (2015)
Majda, A.J., Bertozzi, A.L.: Vorticity and Incompressible Flow. Cambridge University Press, Cambridge (2002)
Natale, A., Cotter, C.J.: A variational H(div) finite-element discretization approach for perfect incompressible fluids. IMA J. Numer. Anal. (2017). https://doi.org/10.1093/imanum/drx033
Oberai, A.A., Liu, J., Sondak, D., Hughes, T.J.R.: A residual based eddy viscosity model for the large eddy simulation of turbulent flows. Comput. Methods Appl. Mech. Eng. 282, 54–70 (2014)
Oikawa, I.: A hybridized discontinuous Galerkin method with reduced stabilization. J. Sci. Comput. 65(1), 327–340 (2015)
Oikawa, I.: Analysis of a reduced-order HDG method for the Stokes equations. J. Sci. Comput. 67(2), 475–492 (2016)
Rhebergen, S., Wells, G.N.: Analysis of a hybridized/interface stabilized finite element method for the Stokes equations. SIAM J. Numer. Anal. 55(4), 1982–2003 (2017)
Rhebergen, S., Wells, G.N.: A hybridizable discontinuous Galerkin method for the Navier-Stokes equations with pointwise divergence-free velocity field. J. Sci. Comput. (2018). https://doi.org/10.1007/s10915-018-0671-4
Rivière, B.: Discontinuous Galerkin Methods for Solving Elliptic and Parabolic Equations. SIAM (2008)
Roos, H.G., Stynes, M., Tobiska, L.: Robust Numerical Methods for Singularly Perturbed Differential Equations: Convection-Diffusion-Reaction and Flow Problems, 2nd edn. Springer, Berlin (2008)
Schlichting, H., Gersten, K.: Boundary-Layer Theory, 8th edn. Springer, Berlin (2000)
Schöberl, J.: C++11 Implementation of Finite Elements in NGSolve. ASC Report 30/2014, Institute for Analysis and Scientific Computing, Vienna University of Technology (2014). https://www.asc.tuwien.ac.at/~schoeberl/wiki/publications/ngs-cpp11.pdf
Schöberl, J., Zaglmayr, S.: High order Nédélec elements with local complete sequence properties. COMPEL 24(2), 374–384 (2005)
Schroeder, P.W., Lube, G.: Divergence-free H(div)-FEM for time-dependent incompressible flows with applications to high Reynolds number vortex dynamics. J. Sci. Comput. 75(2), 830–858 (2018)
Schroeder, P.W., Lube, G.: Pressure–robust analysis of divergence-free and conforming FEM for evolutionary incompressible Navier–Stokes flows. J. Numer. Math. 25(4), 249–276 (2017)
Tritton, D.J.: Physical Fluid Dynamics, 2nd edn. Oxford University Press, New York (1988)
Zaglmayr, S.: High Order Finite Element Methods for Electromagnetic Field Computation. Ph.D. thesis, Johannes Kepler University Linz (2006)
Author information
Authors and Affiliations
Corresponding author
Appendix: Computational aspects of \(\mathbf H \)(div)-conforming methods for Navier–Stokes
Appendix: Computational aspects of \(\mathbf H \)(div)-conforming methods for Navier–Stokes
Improving the efficiency of \({\varvec{H}{{\left( {\mathrm {div}}\right) }}}\)-conforming methods In this section we explain how \({\varvec{H}{{\left( {\mathrm {div}}\right) }}}\)-conforming FE methods, that are often seen as too complicated and inefficient for real application, can be made efficient. We restrict the discussion here to BDM elements as they are computationally more efficient in the context of incompressible flows compared to RT elements since they have less degrees of freedom (DOFs) for the same velocity approximation.
Choosing the pressure space \({Q}_h\) as the space of (discontinuous) piecewise polynomials of one degree less than the \({\varvec{H}{{\left( {\mathrm {div}}\right) }}}\)-conforming velocity space \({\varvec{V}}_h\) renders (16) an equality, that is, \({{\mathrm{\nabla \,\varvec{\cdot }}}}{\varvec{V}}_h = {Q}_h\). A special property of this velocity–pressure pair is that the inf-sup constant is robust in the polynomial degree leading to hp-optimal convergence; cf. [44] for a rigorous analysis in 2D. The strong relation \({{\mathrm{\nabla \,\varvec{\cdot }}}}{\varvec{V}}_h = {Q}_h\) can further be exploited with a smart choice of the basis functions for \({\varvec{V}}_h\) and \({Q}_h\); cf. [63, 67]. The a priori knowledge that the discrete solution will be pointwise divergence-free then allows to remove some DOFs for the velocity and all pressure unknowns except for the piecewise constants; cf. [46, Remark 1] and [45, Section 2.2.4.2]. We make use of this in our numerical experiments.
To account for the tangential discontinuity in the \({\varvec{H}{{\left( {\mathrm {div}}\right) }}}\)-conforming FE space, a DG formulation has to be applied. This aspect can be regarded ambivalently. On the one hand, the discontinuous nature of the tangential component offers the possibility of applying an upwind discretisation for the convection, cf. (22), which results in stable discretisations also in the convective limit [35] without adding too much dissipation compared to most convection stabilisations of \({\varvec{H}^{1}{}}\)-FEM. On the other hand, the DG formulation results in computationally less attractive features. Due to the break-up of the tangential continuity, several DOFs for the velocity are multiplied compared to \({\varvec{H}^{1}{}}\)-conforming methods. Even worse, the number of couplings in a corresponding system matrix increases which results in much higher computational costs for (direct and iterative) solvers of linear systems.
Several measures can be taken to compensate for these costs. To this end, we briefly discuss the concept of hybridisation in the context of DG methods [22]. To reduce the couplings of neighbouring elements, additional unknowns on the facets are introduced (which typically approximate the trace of the unknown field). These additional unknowns are used to replace the direct couplings of neighbouring elements with couplings between element unknowns and the facet unknowns. Due to the lower dimension of the facets, this reduces the overall amount of couplings especially in the higher order case. More importantly, it allows for static condensation, i.e. the elimination of interior unknowns by a local Schur complement strategy which reduces the number of DOFs for which a global linear system needs to be solved.
Depending on the problem at hand there are many ways to make use of hybridisation. For an overview we refer to the review article [18]. For Stokes and Navier–Stokes discretisations many variants have been considered; see, for instance, [19,20,21]. Exactly divergence-free HDG methods have also been considered in [17, 57, 58] where additional facet unknowns can be used to enforce normal continuity on a standard DG space which circumvents the construction of \({\varvec{H}{{\left( {\mathrm {div}}\right) }}}\)-conforming FE spaces. Here, we use the formulation presented in [46] where, additionally to an \({\varvec{H}{{\left( {\mathrm {div}}\right) }}}\)-conforming FE space \({\varvec{V}}_h\) for the velocity and a discontinuous pressure space \({Q}_h\), facet unknowns are introduced only for the tangential component of the velocity. The DG terms in the variational formulation are then adjusted correspondingly. Finally, the element unknowns of the \({\varvec{H}{{\left( {\mathrm {div}}\right) }}}\)-conforming FE space couple with neighbour elements only through facet unknowns. These facet unknowns are either the DOFs for the normal continuity of \({\varvec{V}}_h\) or the additional facet unknowns. All remaining velocity unknowns, as well as the pressure unknowns, have only element local couplings such that these—except for the mean element pressure—can be eliminated during static condensation; cf. Fig. 5 for a sketch.
In the viscosity dominated case hybridisation can be optimised further so that only facet unknowns of one degree less need to be considered; cf. [46, 55, 56]. A similar optimisation can also be made for the unknowns for the normal continuity by relaxing the \({\varvec{H}{{\left( {\mathrm {div}}\right) }}}\)-conformity slightly. We do not treat this here but instead refer to [42]. To make use of these superconvergence properties of HDG methods we apply—as suggested in [46]—an operator splitting time integration method where the convection operator is treated only explicitly while the remaining time-independent operators are treated implicitly. Note that such an operator splitting is not only desirable for hybrid DG discretisations. Several time integration methods allow for such a splitting; cf. [46, Section 3]. For the experiments in Sect. 5.3 a second-order implicit-explicit BDF2 method has been used.
Some performance comparisons for the numerical study in Sect. 5.3 In Sect. 5.3 the errors for Taylor–Hood, Scott–Vogelius, BDM and the hybridised BDM FE discretisation on two different meshes are compared. At this point, this study shall be complemented with information on the computational costs of the methods. The results are shown in Table 1 where we make this comparison only in terms of the following measures. Firstly, the numbers of DOFs for velocity and pressure (\(\#{\left\{ {\varvec{u}}\,{\mathrm {DOFs}} \right\} }\), \(\#{\left\{ p\,{\mathrm {DOFs}} \right\} }\), \(\#{\left\{ {\mathrm {DOFs}} \right\} }\)) are compared. Secondly, we consider the same numbers that remain in a global linear system after static condensation and a potential reduction of the basis (in brackets). Thirdly, the non-zero entries in the global matrix \(M^*\) before (\(\#{\left\{ \text {nz}(M^*) \right\} }\)) and after reduction and static condensation (in brackets) are considered. Note that these numbers can only give an indication of the computational efficiency of the methods. Many different practically relevant aspects, as for example parallelisability or the availability and performance of suitable preconditioners, are not reflected in these numbers.
Regarding static condensation in the Taylor–Hood method, independent of the grad-div stabilisation, we can eliminate all interior unknowns for velocity and pressure. On general meshes, the pressure unknowns for the Scott–Vogelius element cannot be eliminated and hence, static condensation is only applied with respect to the interior velocity DOFs. We note that on barycentre refined meshes static condensation can also be applied for the pressure unknowns; cf. [24]. In case of a DG formulation with BDM elements we utilise the special basis introduced in [63, 67] to eliminate some velocity unknowns and all pressure unknowns except for the mean element pressure. However, static condensation cannot be applied to any additional DOFs due to the DG couplings. Note that this could potentially be improved slightly by choosing a nodal basis similar to the one in [37] where interior unknowns only couple with the boundary nodes of neighbouring elements. To the best of the authors’ knowledge, such a basis has not yet been proposed for an \({\varvec{H}{{\left( {\mathrm {div}}\right) }}}\)-conforming FE space. For the hybridised DG method we can apply the reduction of the basis for the \({\varvec{H}{{\left( {\mathrm {div}}\right) }}}\)-conforming FE space as well as static condensation. Note that in this work, the formulation from [46] is used which only involves tangential facet unknowns of degree 7. The results are shown in Table 1.
We observe that the effect of the basis reduction and especially the hybridisation reduces the computational costs of the \({\varvec{H}{{\left( {\mathrm {div}}\right) }}}\)-conforming methods drastically, thereby rendering them competitive not only in terms of accuracy, cf. Sect. 5.3, but also in terms of computing time; see also the benchmark results in [46, Section 4.5].
Rights and permissions
About this article
Cite this article
Schroeder, P.W., Lehrenfeld, C., Linke, A. et al. Towards computable flows and robust estimates for inf-sup stable FEM applied to the time-dependent incompressible Navier–Stokes equations. SeMA 75, 629–653 (2018). https://doi.org/10.1007/s40324-018-0157-1
Received:
Accepted:
Published:
Issue Date:
DOI: https://doi.org/10.1007/s40324-018-0157-1
Keywords
- Time-dependent incompressible flow
- Re-semi-robust error estimates
- Pressure–robustness
- Inf-sup stable methods
- Exactly divergence-free FEM