Implicit time discretization schemes for mixed least-squares finite element formulations
This work is an extension of the ideas in Averweg et al. (2019) with the focus on a detailed investigation of implicit time discretization schemes to model instationary fluid flow, based on the incompressible Navier–Stokes equations, and linear elastodynamic structural behavior. The variational appr...
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| Published in | Computer methods in applied mechanics and engineering Vol. 368; p. 113111 |
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| Main Authors | , , , |
| Format | Journal Article |
| Language | English |
| Published |
Amsterdam
Elsevier B.V
15.08.2020
Elsevier BV |
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| Online Access | Get full text |
| ISSN | 0045-7825 1879-2138 |
| DOI | 10.1016/j.cma.2020.113111 |
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| Abstract | This work is an extension of the ideas in Averweg et al. (2019) with the focus on a detailed investigation of implicit time discretization schemes to model instationary fluid flow, based on the incompressible Navier–Stokes equations, and linear elastodynamic structural behavior. The variational approaches for fluid and solid mechanics are based on a mixed least-squares finite element method. The L2-norm minimization of the residuals of the constructed first-order systems of the governing differential equations is based on two-field stress–velocity (SV) functionals. For the time discretization of the SV-fluid formulation, four different types of implicit integration schemes are investigated, namely the Houbolt method, the Crank–Nicolson method and two explicit, singly diagonally implicit Runge–Kutta methods (ESDIRK). The SV-formulation for the solid is discretized applying the Houbolt method. The presented time integration schemes are validated investigating an unsteady fluid flow and an elastodynamic structural benchmark. Since both (fluid and solid) SV formulations are discretized using conforming finite element spaces in H(div) and H1, respectively, the inherent fulfillment of coupling conditions, when modeling fluid–structure interaction problems, is given a priori. Therefore, the applicability is also examined by two simplified FSI problems for small deformations, in order to represent the main characteristics of the presented approach.
•Investigation of different implicit time discretizations for mixed least-squares FEM.•Validation and verification for fluid and structure problems.•Accuracy assessment with respect to displacements and lift/drag coefficients.•Application to benchmark problems for FSI problems under small deformations. |
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| AbstractList | This work is an extension of the ideas in Averweg et al. (2019) with the focus on a detailed investigation of implicit time discretization schemes to model instationary fluid flow, based on the incompressible Navier–Stokes equations, and linear elastodynamic structural behavior. The variational approaches for fluid and solid mechanics are based on a mixed least-squares finite element method. The L2-norm minimization of the residuals of the constructed first-order systems of the governing differential equations is based on two-field stress–velocity (SV) functionals. For the time discretization of the SV-fluid formulation, four different types of implicit integration schemes are investigated, namely the Houbolt method, the Crank–Nicolson method and two explicit, singly diagonally implicit Runge–Kutta methods (ESDIRK). The SV-formulation for the solid is discretized applying the Houbolt method. The presented time integration schemes are validated investigating an unsteady fluid flow and an elastodynamic structural benchmark. Since both (fluid and solid) SV formulations are discretized using conforming finite element spaces in H(div) and H1, respectively, the inherent fulfillment of coupling conditions, when modeling fluid–structure interaction problems, is given a priori. Therefore, the applicability is also examined by two simplified FSI problems for small deformations, in order to represent the main characteristics of the presented approach.
•Investigation of different implicit time discretizations for mixed least-squares FEM.•Validation and verification for fluid and structure problems.•Accuracy assessment with respect to displacements and lift/drag coefficients.•Application to benchmark problems for FSI problems under small deformations. This work is an extension of the ideas in Averweg et al. (2019) with the focus on a detailed investigation of implicit time discretization schemes to model instationary fluid flow, based on the incompressible Navier–Stokes equations, and linear elastodynamic structural behavior. The variational approaches for fluid and solid mechanics are based on a mixed least-squares finite element method. The L2-norm minimization of the residuals of the constructed first-order systems of the governing differential equations is based on two-field stress–velocity (SV) functionals. For the time discretization of the SV-fluid formulation, four different types of implicit integration schemes are investigated, namely the Houbolt method, the Crank–Nicolson method and two explicit, singly diagonally implicit Runge–Kutta methods (ESDIRK). The SV-formulation for the solid is discretized applying the Houbolt method. The presented time integration schemes are validated investigating an unsteady fluid flow and an elastodynamic structural benchmark. Since both (fluid and solid) SV formulations are discretized using conforming finite element spaces in H(div) and H1, respectively, the inherent fulfillment of coupling conditions, when modeling fluid–structure interaction problems, is given a priori. Therefore, the applicability is also examined by two simplified FSI problems for small deformations, in order to represent the main characteristics of the presented approach. |
| ArticleNumber | 113111 |
| Author | Schwarz, Alexander Nisters, Carina Schröder, Jörg Averweg, Solveigh |
| Author_xml | – sequence: 1 givenname: Solveigh orcidid: 0000-0002-1396-2343 surname: Averweg fullname: Averweg, Solveigh email: solveigh.averweg@uni-due.de – sequence: 2 givenname: Alexander surname: Schwarz fullname: Schwarz, Alexander email: alexander.schwarz@uni-due.de – sequence: 3 givenname: Carina surname: Nisters fullname: Nisters, Carina email: carina.nisters@uni-due.de – sequence: 4 givenname: Jörg surname: Schröder fullname: Schröder, Jörg email: j.schroeder@uni-due.de |
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| Cites_doi | 10.1007/s11831-007-9006-6 10.1137/0714068 10.1137/S0036142996313592 10.1137/S003614299527299X 10.2514/8.1722 10.1007/BF02127704 10.1115/1.2900803 10.1002/nme.1620260106 10.1016/j.cma.2003.09.006 10.1016/j.jcp.2007.05.005 10.1137/S0036142903422673 10.1002/pamm.201510099 10.1016/0045-7949(89)90315-5 10.1137/S0036142997324976 10.1007/s00466-014-1009-1 10.1002/nme.1620060109 10.1002/fld.3831 10.1016/j.jcp.2005.08.015 10.1007/s00419-012-0638-0 10.1006/jcph.2000.6592 10.1080/1061856031000123580 10.1016/j.compstruc.2006.11.019 10.1007/s00466-017-1395-2 10.1002/fld.2703 10.1016/S0304-3975(97)00067-4 10.1006/jcph.2002.7059 10.1007/s00466-006-0084-3 10.1073/pnas.38.3.235 10.1002/nme.1620080212 10.2140/jomms.2017.12.57 10.1002/pamm.201900204 10.1016/j.cma.2018.01.043 10.1002/nme.1620100505 10.1016/j.medengphy.2005.10.002 10.1016/0045-7825(95)00826-M 10.1016/j.cma.2005.10.007 10.1007/s003660200028 10.1007/s00791-010-0150-4 10.1002/fld.1650180202 10.1016/j.jcp.2003.09.034 10.1016/j.na.2005.01.054 10.1002/fld.1815 10.1016/j.jfluidstructs.2004.06.008 10.1007/3-540-34596-5_7 10.2514/1.22847 10.1002/fld.1650140706 10.1007/s00466-017-1394-3 10.1002/nme.179 |
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| Keywords | Fluid–structure interaction Incompressible Navier–Stokes equations Implicit time discretization schemes Elastodynamics Mixed least-squares finite elements |
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| SubjectTerms | Computational fluid dynamics Differential equations Discretization Elastodynamics Finite element method Fluid flow Fluid–structure interaction Implicit time discretization schemes Incompressible flow Incompressible Navier–Stokes equations Investigations Least squares Mathematical models Mixed least-squares finite elements Runge-Kutta method Solid mechanics Time integration |
| Title | Implicit time discretization schemes for mixed least-squares finite element formulations |
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