A General formulation for the slip velocity boundary condition in lattice Boltzmann methods
Main Author: | |
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Publication Date: | 2024 |
Format: | Conference object |
Language: | por |
Source: | Repositórios Científicos de Acesso Aberto de Portugal (RCAAP) |
Download full: | http://hdl.handle.net/10174/37608 |
Summary: | Numerous fluid flow problems employ the slip velocity boundary condition, which due to their complexity are often only accessible through CFD. While the lattice Boltzmann method (LBM) [1] has been credited as a natural CFD strategy to model the wall slip phenomenon, it is now recognized that numerical artefacts affect the LBM solution [2] if the LBM slip boundary scheme is not properly calibrated. Unfortunately, this calibration uses an ad hoc procedure, and it does not work in general [2]. Currently, the development of consistent LBM slip boundary schemes tends to relate the slip velocity boundary condition with the closure relation of the LBM boundary scheme [2, 3, 4]. In this context, both linkwise or wet-node operation principles can be explored, though none is optimal. In linkwise philosophy [2, 3], boundary populations are constructed along lattice links, making it difficult to handle directional information, like simultaneous satisfaction of the slip (Robin-type) condition for the velocity tangential component and the no-penetration (Dirichlet-type) condition for the velocity normal component. In wet-node philosophy [4], the directional information is naturally handled, but the construction of the boundary populations is more evolving and harder to cope with. This work proposes a scheme that combines these two philosophies. Here, any standard linkwise scheme, e.g. a multireflection scheme [5], can be used to prescribe the no-slip condition over normal and tangential directions, which is amended with a correction term to enforce the conditions for the velocity slip only along the wall tangential direction(s). This correction brings in the information from the first- and second-order velocity derivatives along the pertinent wall directions, which are found in a simple and local way through the LSOB wet-node operation principle [4]. Our theoretical analysis shows that, the proposed mixed linkwise/wet-node scheme, reaches parabolic accuracy for both no-penetration and slip velocity conditions. This high level of accuracy is also confirmed through a series of numerical simulations performed in well-established benchmark test cases of slip flow over planar and curved walls. The comparison of the numerical results here obtained against previously published ones [2, 3, 4] pinpoints the superiority of the present strategy in modelling the slip velocity boundary condition in LBM offering supremacy both in terms of accuracy and simplicity of implementation. |
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A General formulation for the slip velocity boundary condition in lattice Boltzmann methodsLattice Boltzmann MethodsTwo-Relaxation-Time Collision OperatorWall Boundary SchemesSlip Velocity Boundary ConditionsRarefied Gas FlowsNumerous fluid flow problems employ the slip velocity boundary condition, which due to their complexity are often only accessible through CFD. While the lattice Boltzmann method (LBM) [1] has been credited as a natural CFD strategy to model the wall slip phenomenon, it is now recognized that numerical artefacts affect the LBM solution [2] if the LBM slip boundary scheme is not properly calibrated. Unfortunately, this calibration uses an ad hoc procedure, and it does not work in general [2]. Currently, the development of consistent LBM slip boundary schemes tends to relate the slip velocity boundary condition with the closure relation of the LBM boundary scheme [2, 3, 4]. In this context, both linkwise or wet-node operation principles can be explored, though none is optimal. In linkwise philosophy [2, 3], boundary populations are constructed along lattice links, making it difficult to handle directional information, like simultaneous satisfaction of the slip (Robin-type) condition for the velocity tangential component and the no-penetration (Dirichlet-type) condition for the velocity normal component. In wet-node philosophy [4], the directional information is naturally handled, but the construction of the boundary populations is more evolving and harder to cope with. This work proposes a scheme that combines these two philosophies. Here, any standard linkwise scheme, e.g. a multireflection scheme [5], can be used to prescribe the no-slip condition over normal and tangential directions, which is amended with a correction term to enforce the conditions for the velocity slip only along the wall tangential direction(s). This correction brings in the information from the first- and second-order velocity derivatives along the pertinent wall directions, which are found in a simple and local way through the LSOB wet-node operation principle [4]. Our theoretical analysis shows that, the proposed mixed linkwise/wet-node scheme, reaches parabolic accuracy for both no-penetration and slip velocity conditions. This high level of accuracy is also confirmed through a series of numerical simulations performed in well-established benchmark test cases of slip flow over planar and curved walls. The comparison of the numerical results here obtained against previously published ones [2, 3, 4] pinpoints the superiority of the present strategy in modelling the slip velocity boundary condition in LBM offering supremacy both in terms of accuracy and simplicity of implementation.2024-12-19T16:25:18Z2024-12-192024-06-04T00:00:00Zinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/conferenceObjecthttp://hdl.handle.net/10174/37608http://hdl.handle.net/10174/37608porSilva G., A General formulation for the slip velocity boundary condition in lattice Boltzmann methods. 9th European Congress on Computational Methods in Applied Sciences and Engineering – ECCOMAS – 2024, Lisbon, Portugal, 3-7 June, 2024.https://eccomas2024.org/event/contribution/e071b2e1-ae46-11ee-ac5b-000c29ddfc0csimnaonaognsilva@uevora.pt286Silva, Goncaloinfo:eu-repo/semantics/openAccessreponame:Repositórios Científicos de Acesso Aberto de Portugal (RCAAP)instname:FCCN, serviços digitais da FCT – Fundação para a Ciência e a Tecnologiainstacron:RCAAP2024-12-24T01:45:55Zoai:dspace.uevora.pt:10174/37608Portal AgregadorONGhttps://www.rcaap.pt/oai/openaireinfo@rcaap.ptopendoar:https://opendoar.ac.uk/repository/71602025-05-28T19:19:54.828157Repositórios Científicos de Acesso Aberto de Portugal (RCAAP) - FCCN, serviços digitais da FCT – Fundação para a Ciência e a Tecnologiafalse |
dc.title.none.fl_str_mv |
A General formulation for the slip velocity boundary condition in lattice Boltzmann methods |
title |
A General formulation for the slip velocity boundary condition in lattice Boltzmann methods |
spellingShingle |
A General formulation for the slip velocity boundary condition in lattice Boltzmann methods Silva, Goncalo Lattice Boltzmann Methods Two-Relaxation-Time Collision Operator Wall Boundary Schemes Slip Velocity Boundary Conditions Rarefied Gas Flows |
title_short |
A General formulation for the slip velocity boundary condition in lattice Boltzmann methods |
title_full |
A General formulation for the slip velocity boundary condition in lattice Boltzmann methods |
title_fullStr |
A General formulation for the slip velocity boundary condition in lattice Boltzmann methods |
title_full_unstemmed |
A General formulation for the slip velocity boundary condition in lattice Boltzmann methods |
title_sort |
A General formulation for the slip velocity boundary condition in lattice Boltzmann methods |
author |
Silva, Goncalo |
author_facet |
Silva, Goncalo |
author_role |
author |
dc.contributor.author.fl_str_mv |
Silva, Goncalo |
dc.subject.por.fl_str_mv |
Lattice Boltzmann Methods Two-Relaxation-Time Collision Operator Wall Boundary Schemes Slip Velocity Boundary Conditions Rarefied Gas Flows |
topic |
Lattice Boltzmann Methods Two-Relaxation-Time Collision Operator Wall Boundary Schemes Slip Velocity Boundary Conditions Rarefied Gas Flows |
description |
Numerous fluid flow problems employ the slip velocity boundary condition, which due to their complexity are often only accessible through CFD. While the lattice Boltzmann method (LBM) [1] has been credited as a natural CFD strategy to model the wall slip phenomenon, it is now recognized that numerical artefacts affect the LBM solution [2] if the LBM slip boundary scheme is not properly calibrated. Unfortunately, this calibration uses an ad hoc procedure, and it does not work in general [2]. Currently, the development of consistent LBM slip boundary schemes tends to relate the slip velocity boundary condition with the closure relation of the LBM boundary scheme [2, 3, 4]. In this context, both linkwise or wet-node operation principles can be explored, though none is optimal. In linkwise philosophy [2, 3], boundary populations are constructed along lattice links, making it difficult to handle directional information, like simultaneous satisfaction of the slip (Robin-type) condition for the velocity tangential component and the no-penetration (Dirichlet-type) condition for the velocity normal component. In wet-node philosophy [4], the directional information is naturally handled, but the construction of the boundary populations is more evolving and harder to cope with. This work proposes a scheme that combines these two philosophies. Here, any standard linkwise scheme, e.g. a multireflection scheme [5], can be used to prescribe the no-slip condition over normal and tangential directions, which is amended with a correction term to enforce the conditions for the velocity slip only along the wall tangential direction(s). This correction brings in the information from the first- and second-order velocity derivatives along the pertinent wall directions, which are found in a simple and local way through the LSOB wet-node operation principle [4]. Our theoretical analysis shows that, the proposed mixed linkwise/wet-node scheme, reaches parabolic accuracy for both no-penetration and slip velocity conditions. This high level of accuracy is also confirmed through a series of numerical simulations performed in well-established benchmark test cases of slip flow over planar and curved walls. The comparison of the numerical results here obtained against previously published ones [2, 3, 4] pinpoints the superiority of the present strategy in modelling the slip velocity boundary condition in LBM offering supremacy both in terms of accuracy and simplicity of implementation. |
publishDate |
2024 |
dc.date.none.fl_str_mv |
2024-12-19T16:25:18Z 2024-12-19 2024-06-04T00:00:00Z |
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info:eu-repo/semantics/publishedVersion |
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http://hdl.handle.net/10174/37608 http://hdl.handle.net/10174/37608 |
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http://hdl.handle.net/10174/37608 |
dc.language.iso.fl_str_mv |
por |
language |
por |
dc.relation.none.fl_str_mv |
Silva G., A General formulation for the slip velocity boundary condition in lattice Boltzmann methods. 9th European Congress on Computational Methods in Applied Sciences and Engineering – ECCOMAS – 2024, Lisbon, Portugal, 3-7 June, 2024. https://eccomas2024.org/event/contribution/e071b2e1-ae46-11ee-ac5b-000c29ddfc0c sim nao nao gnsilva@uevora.pt 286 |
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info:eu-repo/semantics/openAccess |
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openAccess |
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