A finite-difference ghost-point multigrid method for multi-scale modelling of sorption kinetics of a surfactant past an oscillating bubble
We propose a method for the numerical solution of a multiscale model describing sorption kinetics of a surfactant around an oscillating bubble. The evolution of the particles is governed by a convection-diffusion equation for the surfactant concentration \(c\), with suitable boundary condition on th...
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description | We propose a method for the numerical solution of a multiscale model describing sorption kinetics of a surfactant around an oscillating bubble. The evolution of the particles is governed by a convection-diffusion equation for the surfactant concentration \(c\), with suitable boundary condition on the bubble surface, which models the action of the short range attractive-repulsive potential acting on them when they get sufficiently close to the surface \cite{multiscale_mod}. In the domain occupied by the fluid, the particles are transported by the fluid motion generated by the bubble oscillations. The method adopted to solve the equation for \(c\) is based on a finite-difference scheme on a uniform Cartesian grid and implemented in 2D and 3D axisymmetric domains. We use a level-set function to define the region occupied by the bubble, while the boundary conditions are discretized by a ghost-point technique to guarantee second order accuracy at the curved boundary. The sparse linear system is finally solved with a geometric multigrid technique designed \textit{ad-hoc\/} for this specific problem. Several accuracy tests are provided to prove second order accuracy in space and time. The fluid dynamics generated by the oscillating bubble is governed by the Stokes equation solved with a second order accurate method based on a monolithic approach, where the momentum and continuity equations are solved simultaneously. Since the amplitude of the bubble oscillations are very small, a simplified model is presented where the computational bubble is actually steady and its oscillations are represented purely with time-dependent boundary conditions. A numerical comparison with the moving domain model confirms that this simplification is perfectly reasonable for the class of problems investigated in this paper. |
doi_str_mv | 10.48550/arxiv.2206.02491 |
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The evolution of the particles is governed by a convection-diffusion equation for the surfactant concentration \(c\), with suitable boundary condition on the bubble surface, which models the action of the short range attractive-repulsive potential acting on them when they get sufficiently close to the surface \cite{multiscale_mod}. In the domain occupied by the fluid, the particles are transported by the fluid motion generated by the bubble oscillations. The method adopted to solve the equation for \(c\) is based on a finite-difference scheme on a uniform Cartesian grid and implemented in 2D and 3D axisymmetric domains. We use a level-set function to define the region occupied by the bubble, while the boundary conditions are discretized by a ghost-point technique to guarantee second order accuracy at the curved boundary. The sparse linear system is finally solved with a geometric multigrid technique designed \textit{ad-hoc\/} for this specific problem. Several accuracy tests are provided to prove second order accuracy in space and time. The fluid dynamics generated by the oscillating bubble is governed by the Stokes equation solved with a second order accurate method based on a monolithic approach, where the momentum and continuity equations are solved simultaneously. Since the amplitude of the bubble oscillations are very small, a simplified model is presented where the computational bubble is actually steady and its oscillations are represented purely with time-dependent boundary conditions. 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Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><rights>http://creativecommons.org/licenses/by/4.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,780,784,885,27924</link.rule.ids><backlink>$$Uhttps://doi.org/10.48550/arXiv.2206.02491$$DView paper in arXiv$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.1016/j.jcp.2022.111880$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink></links><search><creatorcontrib>Astuto, Clarissa</creatorcontrib><creatorcontrib>Coco, Armando</creatorcontrib><creatorcontrib>Russo, Giovanni</creatorcontrib><title>A finite-difference ghost-point multigrid method for multi-scale modelling of sorption kinetics of a surfactant past an oscillating bubble</title><title>arXiv.org</title><description>We propose a method for the numerical solution of a multiscale model describing sorption kinetics of a surfactant around an oscillating bubble. The evolution of the particles is governed by a convection-diffusion equation for the surfactant concentration \(c\), with suitable boundary condition on the bubble surface, which models the action of the short range attractive-repulsive potential acting on them when they get sufficiently close to the surface \cite{multiscale_mod}. In the domain occupied by the fluid, the particles are transported by the fluid motion generated by the bubble oscillations. The method adopted to solve the equation for \(c\) is based on a finite-difference scheme on a uniform Cartesian grid and implemented in 2D and 3D axisymmetric domains. We use a level-set function to define the region occupied by the bubble, while the boundary conditions are discretized by a ghost-point technique to guarantee second order accuracy at the curved boundary. The sparse linear system is finally solved with a geometric multigrid technique designed \textit{ad-hoc\/} for this specific problem. Several accuracy tests are provided to prove second order accuracy in space and time. The fluid dynamics generated by the oscillating bubble is governed by the Stokes equation solved with a second order accurate method based on a monolithic approach, where the momentum and continuity equations are solved simultaneously. Since the amplitude of the bubble oscillations are very small, a simplified model is presented where the computational bubble is actually steady and its oscillations are represented purely with time-dependent boundary conditions. A numerical comparison with the moving domain model confirms that this simplification is perfectly reasonable for the class of problems investigated in this paper.</description><subject>Accuracy</subject><subject>Boundary conditions</subject><subject>Cartesian coordinates</subject><subject>Computer Science - Numerical Analysis</subject><subject>Continuity equation</subject><subject>Convection-diffusion equation</subject><subject>Domains</subject><subject>Finite difference method</subject><subject>Fluid dynamics</subject><subject>Kinetics</subject><subject>Mathematical analysis</subject><subject>Mathematical models</subject><subject>Mathematics - Numerical Analysis</subject><subject>Oscillations</subject><subject>Sorption</subject><subject>Surfactants</subject><subject>Time dependence</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GOX</sourceid><recordid>eNotkM1qwzAQhEWh0JDmAXqqoGensuSf-BhC_yDQS-5mrZUSpbLkSnJpX6FPXSfpaWCYHXY-Qu5ytixWZckeIXybryXnrFoyXjT5FZlxIfJsVXB-QxYxHhljvKp5WYoZ-V1TbZxJKkOjtQrKSUX3Bx9TNnjjEu1Hm8w-GKS9SgePVPtwMbMowSrae1TWGrenXtPow5CMd_TDOJWMjCcTaByDBplg6hsgJgqO-iiNtZBOh93YdVbdkmsNNqrFv87J7vlpt3nNtu8vb5v1NoOmzDOOouiwq3EaoBkHxIpLrDsUiq0KXeeCYSOFhhyg5FKjhLKqRSFQNlpiJ-bk_lJ7BtUOwfQQftoTsPYMbEo8XBJD8J-jiqk9-jG46ad24iZq1jSiFn9OfnJT</recordid><startdate>20220606</startdate><enddate>20220606</enddate><creator>Astuto, Clarissa</creator><creator>Coco, Armando</creator><creator>Russo, Giovanni</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>AKY</scope><scope>AKZ</scope><scope>GOX</scope></search><sort><creationdate>20220606</creationdate><title>A finite-difference ghost-point multigrid method for multi-scale modelling of sorption kinetics of a surfactant past an oscillating bubble</title><author>Astuto, Clarissa ; Coco, Armando ; Russo, Giovanni</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a951-2d34bdb7d725f02add62cd7bd3e084f7130d9c3fa1aa52cfdca567343dc9fcdb3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Accuracy</topic><topic>Boundary conditions</topic><topic>Cartesian coordinates</topic><topic>Computer Science - Numerical Analysis</topic><topic>Continuity equation</topic><topic>Convection-diffusion equation</topic><topic>Domains</topic><topic>Finite difference method</topic><topic>Fluid dynamics</topic><topic>Kinetics</topic><topic>Mathematical analysis</topic><topic>Mathematical models</topic><topic>Mathematics - Numerical Analysis</topic><topic>Oscillations</topic><topic>Sorption</topic><topic>Surfactants</topic><topic>Time dependence</topic><toplevel>online_resources</toplevel><creatorcontrib>Astuto, Clarissa</creatorcontrib><creatorcontrib>Coco, Armando</creatorcontrib><creatorcontrib>Russo, Giovanni</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection (ProQuest)</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering Collection</collection><collection>arXiv Computer Science</collection><collection>arXiv Mathematics</collection><collection>arXiv.org</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Astuto, Clarissa</au><au>Coco, Armando</au><au>Russo, Giovanni</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>A finite-difference ghost-point multigrid method for multi-scale modelling of sorption kinetics of a surfactant past an oscillating bubble</atitle><jtitle>arXiv.org</jtitle><date>2022-06-06</date><risdate>2022</risdate><eissn>2331-8422</eissn><abstract>We propose a method for the numerical solution of a multiscale model describing sorption kinetics of a surfactant around an oscillating bubble. The evolution of the particles is governed by a convection-diffusion equation for the surfactant concentration \(c\), with suitable boundary condition on the bubble surface, which models the action of the short range attractive-repulsive potential acting on them when they get sufficiently close to the surface \cite{multiscale_mod}. In the domain occupied by the fluid, the particles are transported by the fluid motion generated by the bubble oscillations. The method adopted to solve the equation for \(c\) is based on a finite-difference scheme on a uniform Cartesian grid and implemented in 2D and 3D axisymmetric domains. We use a level-set function to define the region occupied by the bubble, while the boundary conditions are discretized by a ghost-point technique to guarantee second order accuracy at the curved boundary. The sparse linear system is finally solved with a geometric multigrid technique designed \textit{ad-hoc\/} for this specific problem. Several accuracy tests are provided to prove second order accuracy in space and time. The fluid dynamics generated by the oscillating bubble is governed by the Stokes equation solved with a second order accurate method based on a monolithic approach, where the momentum and continuity equations are solved simultaneously. Since the amplitude of the bubble oscillations are very small, a simplified model is presented where the computational bubble is actually steady and its oscillations are represented purely with time-dependent boundary conditions. A numerical comparison with the moving domain model confirms that this simplification is perfectly reasonable for the class of problems investigated in this paper.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.2206.02491</doi><oa>free_for_read</oa></addata></record> |
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subjects | Accuracy Boundary conditions Cartesian coordinates Computer Science - Numerical Analysis Continuity equation Convection-diffusion equation Domains Finite difference method Fluid dynamics Kinetics Mathematical analysis Mathematical models Mathematics - Numerical Analysis Oscillations Sorption Surfactants Time dependence |
title | A finite-difference ghost-point multigrid method for multi-scale modelling of sorption kinetics of a surfactant past an oscillating bubble |
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