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A geometric multigrid method for space-time finite element discretizations of the Navier-Stokes equations and its application to 3d flow simulation
Numerical Analysis · Submitted 22 Jul 2021
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Its performance properties are demonstrated for 2d and 3d benchmarks of flow around a cylinder.
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The abstract, sentence by sentence
We present a parallelized geometric multigrid (GMG) method, based on the cell-based Vanka smoother, for higher order space-time finite element methods (STFEM) to the incompressible Navier--Stokes equations. The STFEM is implemented as a time marching scheme. The GMG solver is applied as a preconditioner for GMRES iterations. Its performance properties are demonstrated for 2d and 3d benchmarks of flow around a cylinder. The key ingredients of the GMG approach are the construction of the local Vanka smoother over all degrees of freedom in time of the respective subinterval and its efficient application. For this, data structures that store pre-computed cell inverses of the Jacobian for all hierarchical levels and require only a reasonable amount of memory overhead are generated. The GMG method is built for the \emph{deal.II} finite element library. The concepts are flexible and can be transferred to similar software platforms.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present a parallelized geometric multigrid (GMG) method, based on the cell-based Vanka smoother, for higher order space-time finite element methods (STFEM) to the incompressible Navier--Stokes equations. | contribution 0.98 | 0.94 | 0.21 | asserted 1.00 |
| s1 | The STFEM is implemented as a time marching scheme. | method 0.98 | 0.80 | 0.03 | asserted 1.00 |
| s2 | The GMG solver is applied as a preconditioner for GMRES iterations. | method 0.98 | 0.81 | 0.07 | asserted 1.00 |
| s3 | Its performance properties are demonstrated for 2d and 3d benchmarks of flow around a cylinder. | result 0.77 | 0.93 | 0.19 | asserted 1.00 |
| s4 | The key ingredients of the GMG approach are the construction of the local Vanka smoother over all degrees of freedom in time of the respective subinterval and its efficient application. | method 0.86 | 0.84 | 0.13 | asserted 1.00 |
| s5 | For this, data structures that store pre-computed cell inverses of the Jacobian for all hierarchical levels and require only a reasonable amount of memory overhead are generated. | method 0.98 | 0.89 | 0.04 | asserted 1.00 |
| s6 | The GMG method is built for the \emph{deal.II} finite element library. | method 0.80 | 0.80 | 0.03 | asserted 1.00 |
| s7 | The concepts are flexible and can be transferred to similar software platforms. | interpretation 0.49 | 0.37 | 0.06 | asserted 0.59 |
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The paper
Original abstract
We present a parallelized geometric multigrid (GMG) method, based on the cell-based Vanka smoother, for higher order space-time finite element methods (STFEM) to the incompressible Navier--Stokes equations. The STFEM is implemented as a time marching scheme. The GMG solver is applied as a preconditioner for GMRES iterations. Its performance properties are demonstrated for 2d and 3d benchmarks of flow around a cylinder. The key ingredients of the GMG approach are the construction of the local Vanka smoother over all degrees of freedom in time of the respective subinterval and its efficient application. For this, data structures that store pre-computed cell inverses of the Jacobian for all hierarchical levels and require only a reasonable amount of memory overhead are generated. The GMG method is built for the \emph{deal.II} finite element library. The concepts are flexible and can be transferred to similar software platforms.
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How the literature uses it
3 arXiv papers cite this in 21 sentences
Papers whose main result relates to this one's
States the same result 1 paper
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We demonstrate numerically the efficiency of preconditioning GMRES iterations for solving these linear systems by a $V$-cycle geometric multigrid approach based on a local Vanka smoother.
Papers citing it · 16 sentences without a confident label
Uses its method or tool 2 papers
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For details of the parallel implementation of the geometric multigrid solver we refer to [ref] .
An energy-efficient GMRES-Multigrid solver for space-time finite element computation of dynamic poro- and thermoelasticity · Numerical studies · 0.80
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The implementation of the numerical scheme was done in an in-house high-performance frontend solver for the library [ref] .
Convergence of a continuous Galerkin method for hyperbolic-parabolic systems · Numerical convergence test · 0.99
Compares with it 1 paper
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This is in contrast to the Navier–Stokes equations for which elementwise Vanka-type smoother are known to perform excellently if discontinuous pressure approximations are applied; cf. [ref] .
An energy-efficient GMRES-Multigrid solver for space-time finite element computation of dynamic poro- and thermoelasticity · Space-time finite element and multigrid techniques · 0.80
Cites it as support 1 paper
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Numerical evidence of these performance properties is presented in, e.g., [ref] .
Efficiency of local Vanka smoother geometric multigrid preconditioning for space-time finite element methods to the Navier-Stokes equations · Introduction · 0.99
Cites it as background 1 paper
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For this we refer to, e.g., [ref] and the references therein.
Efficiency of local Vanka smoother geometric multigrid preconditioning for space-time finite element methods to the Navier-Stokes equations · Introduction · 0.94
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