Discontinuous Galerkin simulator of shallow vortical flow with turbulence

• Discontinuous Galerkin solver of the RANS equations with the k- ε model (RANS -k- ε). • Solving an enlarged set of thirteen advection-dominated RANS -k- ε equations. • New treatments for preserving the stability and positivity of the turbulent-flow variables. • Open-source integration on LISFLOOD-FP for parallel CPU or GPU simulations. • Reliable predictions of various vortical flow types in laminar and turbulent regimes. Shallow vortical flow can often occurs past (un)submerged topographies, prevailing in quasi-steady states with turbulence. Practically, vortical flow is represented by the two-dimensional (2D) Reynolds-Averaged Navier–Stokes equations, including the two-equation k- ε turbulent model (RANS- k- ε), and are commonly resolved by finite difference/volumes second-order accurate solvers. Such RANS- k- ε solvers, in addition to needing a fine resolution, require adding artificial treatments–extrinsic (unlocalised) reconstructions of wet-dry fronts with slope-limiting–that can impact the vortical eddy predictions. The second-order discontinuous Galerkin (DG2) solver intrinsically integrates the wet-dry fronts and uses localised slope-limiting; resulting in an implicit large eddy simulator with the shallow water equations (DG2-SWE) that can only simulate uncompounded eddies. A novel DG2 solver of RANS- k- ε (DG2-RANS- k- ε) is devised for simulating a wider range of vortical eddies, by: first, transforming the 5×5 advective-diffusive RANS- k- ε system into a 13×13 advection-dominated system; second, extending the DG2 formulation to the 13×13 system, with adaptation of its robustness treatments for the mean-flow variables; and, last, adding a new combination of stability/positivity-preserving treatments for turbulent-flow quantities. The DG2-RANS -k- ε solver is evaluated for simulating five experimental benchmarks using coarse, medium and fine resolutions. Results show that DG2-RANS -k- ε can reproduce compound eddies from the medium resolution, and that DG2-RANS (without k- ε) can better reproduce laminar wakes. Using the medium resolution reduces runtimes by 7-fold and running on the GPU further reduce runtimes by 2-to-6-fold. The code, including simulation setup files, is open-source within a new release of the LISFLOOD-FP hydraulic modelling environment (https://doi.org/10.5281/zenodo.7628739), with documentation and demonstration videos ( https://www.seamlesswave.com/DG2_RANS ).

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Publication Details

Journal
Advances in Water Resources
Published
2025-04-14
DOI
https://doi.org/10.1016/j.advwatres.2025.104986
Primary Topic
Computational Fluid Dynamics and Aerodynamics
Type
article
Field-Weighted Citation Impact
0.00

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article

Discontinuous Galerkin simulator of shallow vortical flow with turbulence

Georges Kesserwani, Mahya Hajihassanpour, Mohammad Kazem Sharifian, Xitong Sun
Advances in Water Resources
Computational Fluid Dynamics and Aerodynamics
article

Discontinuous Galerkin simulator of shallow vortical flow with turbulence

Georges Kesserwani, Mahya Hajihassanpour, Mohammad Kazem Sharifian, Xitong Sun
article en

Abstract

• Discontinuous Galerkin solver of the RANS equations with the k- ε model (RANS -k- ε). • Solving an enlarged set of thirteen advection-dominated RANS -k- ε equations. • New treatments for preserving the stability and positivity of the turbulent-flow variables. • Open-source integration on LISFLOOD-FP for parallel CPU or GPU simulations. • Reliable predictions of various vortical flow types in laminar and turbulent regimes. Shallow vortical flow can often occurs past (un)submerged topographies, prevailing in quasi-steady states with turbulence. Practically, vortical flow is represented by the two-dimensional (2D) Reynolds-Averaged Navier–Stokes equations, including the two-equation k- ε turbulent model (RANS- k- ε), and are commonly resolved by finite difference/volumes second-order accurate solvers. Such RANS- k- ε solvers, in addition to needing a fine resolution, require adding artificial treatments–extrinsic (unlocalised) reconstructions of wet-dry fronts with slope-limiting–that can impact the vortical eddy predictions. The second-order discontinuous Galerkin (DG2) solver intrinsically integrates the wet-dry fronts and uses localised slope-limiting; resulting in an implicit large eddy simulator with the shallow water equations (DG2-SWE) that can only simulate uncompounded eddies. A novel DG2 solver of RANS- k- ε (DG2-RANS- k- ε) is devised for simulating a wider range of vortical eddies, by: first, transforming the 5×5 advective-diffusive RANS- k- ε system into a 13×13 advection-dominated system; second, extending the DG2 formulation to the 13×13 system, with adaptation of its robustness treatments for the mean-flow variables; and, last, adding a new combination of stability/positivity-preserving treatments for turbulent-flow quantities. The DG2-RANS -k- ε solver is evaluated for simulating five experimental benchmarks using coarse, medium and fine resolutions. Results show that DG2-RANS -k- ε can reproduce compound eddies from the medium resolution, and that DG2-RANS (without k- ε) can better reproduce laminar wakes. Using the medium resolution reduces runtimes by 7-fold and running on the GPU further reduce runtimes by 2-to-6-fold. The code, including simulation setup files, is open-source within a new release of the LISFLOOD-FP hydraulic modelling environment (https://doi.org/10.5281/zenodo.7628739), with documentation and demonstration videos ( https://www.seamlesswave.com/DG2_RANS ).

Advances in Water ResourcesVol. 201
University of Sheffield (GB)
Engineering and Physical Sciences Research Council
Openalex Percentile: Top 91%
Computational Fluid Dynamics and Aerodynamics
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