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Key ingredients for wall-modeled LES with the Lattice Boltzmann method: Systematic comparison of collision schemes, SGS models, and wall functions on simulation accuracy and efficiency for turbulent channel flow

Spinelli, Gregorio Gerardo und Gericke, Jana und Masilamani, Kannan und Klimach, Harald Günther (2023) Key ingredients for wall-modeled LES with the Lattice Boltzmann method: Systematic comparison of collision schemes, SGS models, and wall functions on simulation accuracy and efficiency for turbulent channel flow. Discrete and Continuous Dynamical Systems - Series S, Seiten 1-28. American Institute of Mathematical Sciences. doi: 10.3934/dcdss.2023212. ISSN 1937-1632.

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Offizielle URL: https://www.aimsciences.org/article/doi/10.3934/dcdss.2023212

Kurzfassung

In this study, we consider different combinations of collision schemes, wall functions, and subgrid scale (SGS) models to simulate the bi-periodic turbulent channel flow at . The study is carried out on a lattice stencil, where the considered collision schemes are the Multiple Relaxation Times (MRT), the Hybrid Recursive Regularized Bhatnagar-Gross-Krook (HRR), and the parameterized Cumulant scheme. The considered SGS models are the Smagorinsky, the Wall-Adapting Local Eddy-viscosity (WALE), and the Vreman model. The Cumulant scheme utilizes its intrinsic implicit SGS model. The turbulent velocity profile is modeled with the following wall functions: the Reichardt, the Musker, and a combination of the Werner and Wengle and the Schmitt (Power-law) function. To assure an impartial comparison, all these ingredients are implemented in the same infrastructure, the open-source software Musubi. The comparison of the considered wall functions shows that the Musker function offers a good compromise between accuracy and performance. When comparing the considered SGS models, although the WALE model delivers the most accurate results, the Vreman model offers the fastest computation. On average, the parallel performance improves by . Amongst the considered collision schemes, the Cumulant outperforms the competitors accuracy-wise. However, for the considered test case, the fastest collision scheme is the MRT. Our investigations show that for the considered test case, the best results in terms of accuracy and performance are delivered by the combination of the Cumulant scheme with its implicit SGS model and the Musker wall function.

elib-URL des Eintrags:https://elib.dlr.de/202169/
Dokumentart:Zeitschriftenbeitrag
Titel:Key ingredients for wall-modeled LES with the Lattice Boltzmann method: Systematic comparison of collision schemes, SGS models, and wall functions on simulation accuracy and efficiency for turbulent channel flow
Autoren:
AutorenInstitution oder E-Mail-AdresseAutoren-ORCID-iDORCID Put Code
Spinelli, Gregorio GerardoGregorioGerardo.Spinelli (at) dlr.dehttps://orcid.org/0000-0001-6578-2494NICHT SPEZIFIZIERT
Gericke, Janajana.gericke (at) dlr.dehttps://orcid.org/0000-0003-0322-2197151823602
Masilamani, KannanKannan.Masilamani (at) dlr.dehttps://orcid.org/0000-0002-3640-2154NICHT SPEZIFIZIERT
Klimach, Harald Güntherharald.klimach (at) dlr.dehttps://orcid.org/0000-0002-6054-5681151823603
Datum:Dezember 2023
Erschienen in:Discrete and Continuous Dynamical Systems - Series S
Referierte Publikation:Ja
Open Access:Ja
Gold Open Access:Nein
In SCOPUS:Ja
In ISI Web of Science:Ja
DOI:10.3934/dcdss.2023212
Seitenbereich:Seiten 1-28
Verlag:American Institute of Mathematical Sciences
ISSN:1937-1632
Status:veröffentlicht
Stichwörter:Lattice Boltzmann method, Hybrid recursive regularized BGK, Cumulant, turbulence modeling, Musubi, wall functions
HGF - Forschungsbereich:Luftfahrt, Raumfahrt und Verkehr
HGF - Programm:Luftfahrt
HGF - Programmthema:keine Zuordnung
DLR - Schwerpunkt:Luftfahrt
DLR - Forschungsgebiet:L - keine Zuordnung
DLR - Teilgebiet (Projekt, Vorhaben):L - keine Zuordnung
Standort: Dresden
Institute & Einrichtungen:Institut für Softwaremethoden zur Produkt-Virtualisierung
Hinterlegt von: Gericke, Jana
Hinterlegt am:29 Jan 2024 12:26
Letzte Änderung:01 Jul 2024 13:08

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