Lattice Boltzmann simulations of contact line motion in a liquid-gas system
We use a lattice Boltzmann algorithm for liquid-gas coexistence to investigate the steady state interface profile of a droplet held between two shearing walls. The algorithm solves the hydrodynamic equations of motion for the system. Partial wetting at the walls is implemented to agree with Cahn the...
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creator | Briant, A. J Papatzacos, P Yeomans, J. M |
description | We use a lattice Boltzmann algorithm for liquid-gas coexistence to
investigate the steady state interface profile of a droplet held between two
shearing walls. The algorithm solves the hydrodynamic equations of motion for
the system. Partial wetting at the walls is implemented to agree with Cahn
theory. This allows us to investigate the processes which lead to the motion of
the three-phase contact line. We confirm that the profiles are a function of
the capillary number and a finite size analysis shows the emergence of a
dynamic contact angle, which can be defined in a region where the interfacial
curvature tends to zero. |
doi_str_mv | 10.48550/arxiv.cond-mat/0203093 |
format | Article |
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investigate the steady state interface profile of a droplet held between two
shearing walls. The algorithm solves the hydrodynamic equations of motion for
the system. Partial wetting at the walls is implemented to agree with Cahn
theory. This allows us to investigate the processes which lead to the motion of
the three-phase contact line. We confirm that the profiles are a function of
the capillary number and a finite size analysis shows the emergence of a
dynamic contact angle, which can be defined in a region where the interfacial
curvature tends to zero.</description><identifier>DOI: 10.48550/arxiv.cond-mat/0203093</identifier><language>eng</language><subject>Physics - Soft Condensed Matter ; Physics - Statistical Mechanics</subject><creationdate>2002-03</creationdate><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,780,885</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/cond-mat/0203093$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.48550/arXiv.cond-mat/0203093$$DView paper in arXiv$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.1098/rsta.2001.0943$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink></links><search><creatorcontrib>Briant, A. J</creatorcontrib><creatorcontrib>Papatzacos, P</creatorcontrib><creatorcontrib>Yeomans, J. M</creatorcontrib><title>Lattice Boltzmann simulations of contact line motion in a liquid-gas system</title><description>We use a lattice Boltzmann algorithm for liquid-gas coexistence to
investigate the steady state interface profile of a droplet held between two
shearing walls. The algorithm solves the hydrodynamic equations of motion for
the system. Partial wetting at the walls is implemented to agree with Cahn
theory. This allows us to investigate the processes which lead to the motion of
the three-phase contact line. We confirm that the profiles are a function of
the capillary number and a finite size analysis shows the emergence of a
dynamic contact angle, which can be defined in a region where the interfacial
curvature tends to zero.</description><subject>Physics - Soft Condensed Matter</subject><subject>Physics - Statistical Mechanics</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2002</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNqNjr0KwkAQhK-xEPUZ3MYyyekZ0FZRBC3tjyW5hIX70dxGjE9vInkAq4GPGeYTYrmW6XaX5zLD5k2vtAi-TBxyJjdSyb2aiusNmakwcAiWPw69h0iutcgUfIRQQb9hLBgseQMuDBzIA_bg2VKZ1BghdpGNm4tJhTaaxZgzsTqf7sdL8jvXj4YcNp0eJHQvoUcJ9W_vCx_tQ4E</recordid><startdate>20020305</startdate><enddate>20020305</enddate><creator>Briant, A. J</creator><creator>Papatzacos, P</creator><creator>Yeomans, J. M</creator><scope>GOX</scope></search><sort><creationdate>20020305</creationdate><title>Lattice Boltzmann simulations of contact line motion in a liquid-gas system</title><author>Briant, A. J ; Papatzacos, P ; Yeomans, J. M</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-arxiv_primary_cond_mat_02030933</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2002</creationdate><topic>Physics - Soft Condensed Matter</topic><topic>Physics - Statistical Mechanics</topic><toplevel>online_resources</toplevel><creatorcontrib>Briant, A. J</creatorcontrib><creatorcontrib>Papatzacos, P</creatorcontrib><creatorcontrib>Yeomans, J. M</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Briant, A. J</au><au>Papatzacos, P</au><au>Yeomans, J. M</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Lattice Boltzmann simulations of contact line motion in a liquid-gas system</atitle><date>2002-03-05</date><risdate>2002</risdate><abstract>We use a lattice Boltzmann algorithm for liquid-gas coexistence to
investigate the steady state interface profile of a droplet held between two
shearing walls. The algorithm solves the hydrodynamic equations of motion for
the system. Partial wetting at the walls is implemented to agree with Cahn
theory. This allows us to investigate the processes which lead to the motion of
the three-phase contact line. We confirm that the profiles are a function of
the capillary number and a finite size analysis shows the emergence of a
dynamic contact angle, which can be defined in a region where the interfacial
curvature tends to zero.</abstract><doi>10.48550/arxiv.cond-mat/0203093</doi><oa>free_for_read</oa></addata></record> |
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subjects | Physics - Soft Condensed Matter Physics - Statistical Mechanics |
title | Lattice Boltzmann simulations of contact line motion in a liquid-gas system |
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