Modeling interfacial mass transfer driven bubble growth in supersaturated solutions

A commonly encountered phenomenon in chemical processes is bubble evolution driven by supersaturation. On the continuum scale, this essentially involves interfacial mass transfer resulting in the growth of bubbles and their subsequent detachment from a surface. Analytical approaches to study this ph...

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Main Authors: Kurian J. Vachaparambil, Kristian Etienne Einarsrud
Format: Article
Language:English
Published: AIP Publishing LLC 2020-10-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/5.0020210
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spelling doaj-a7ba923ca1e6429e93699461faf85a492020-11-25T03:06:28ZengAIP Publishing LLCAIP Advances2158-32262020-10-011010105024105024-910.1063/5.0020210Modeling interfacial mass transfer driven bubble growth in supersaturated solutionsKurian J. Vachaparambil0Kristian Etienne Einarsrud1Department of Materials Science and Engineering, Norwegian University of Science and Technology (NTNU), Trondheim 7491, NorwayDepartment of Materials Science and Engineering, Norwegian University of Science and Technology (NTNU), Trondheim 7491, NorwayA commonly encountered phenomenon in chemical processes is bubble evolution driven by supersaturation. On the continuum scale, this essentially involves interfacial mass transfer resulting in the growth of bubbles and their subsequent detachment from a surface. Analytical approaches to study this phenomenon typically involve estimating the driving force for interfacial mass transfer based on Sherwood number (Sh) correlations and the bulk concentration of dissolved gas. This is often not practical since the bulk concentration is often unknown and Sh correlations are sometimes not available to provide an accurate description of the associated flow fields. With the use of interface-resolved simulations to model these processes, the local distribution of dissolved gas can be obtained by solving for the concentration field. The driving force for interfacial mass transfer can be computed based on Sh correlations (which can be adopted for specific flows and are typically used in “engineering” applications) or the universally applicable Fick’s first law. This paper compares the predictions of these approaches for the well-studied case of a two-dimensional bubble growing in an unbounded supersaturated solution for three different levels of supersaturation. The equivalent two-dimensional simulations are run in a previously developed volume of fluid framework on OpenFOAM® [K. J. Vachaparambil and K. E. Einarsrud, Appl. Math. Model. 81, 690–710 (2020)]. The results show that the choice of an appropriate Sh correlation can provide a reasonable estimate of bubble growth. In a more universal approach, which is relevant when the flow being simulated cannot be captured by a single Sh correlation (e.g., bubble growth/coalescence and detachment) or when existing Sh correlations are not applicable, Fick’s first law can be used to compute the driving force for bubble growth, provided that the concentration boundary layer can be resolved.http://dx.doi.org/10.1063/5.0020210
collection DOAJ
language English
format Article
sources DOAJ
author Kurian J. Vachaparambil
Kristian Etienne Einarsrud
spellingShingle Kurian J. Vachaparambil
Kristian Etienne Einarsrud
Modeling interfacial mass transfer driven bubble growth in supersaturated solutions
AIP Advances
author_facet Kurian J. Vachaparambil
Kristian Etienne Einarsrud
author_sort Kurian J. Vachaparambil
title Modeling interfacial mass transfer driven bubble growth in supersaturated solutions
title_short Modeling interfacial mass transfer driven bubble growth in supersaturated solutions
title_full Modeling interfacial mass transfer driven bubble growth in supersaturated solutions
title_fullStr Modeling interfacial mass transfer driven bubble growth in supersaturated solutions
title_full_unstemmed Modeling interfacial mass transfer driven bubble growth in supersaturated solutions
title_sort modeling interfacial mass transfer driven bubble growth in supersaturated solutions
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2020-10-01
description A commonly encountered phenomenon in chemical processes is bubble evolution driven by supersaturation. On the continuum scale, this essentially involves interfacial mass transfer resulting in the growth of bubbles and their subsequent detachment from a surface. Analytical approaches to study this phenomenon typically involve estimating the driving force for interfacial mass transfer based on Sherwood number (Sh) correlations and the bulk concentration of dissolved gas. This is often not practical since the bulk concentration is often unknown and Sh correlations are sometimes not available to provide an accurate description of the associated flow fields. With the use of interface-resolved simulations to model these processes, the local distribution of dissolved gas can be obtained by solving for the concentration field. The driving force for interfacial mass transfer can be computed based on Sh correlations (which can be adopted for specific flows and are typically used in “engineering” applications) or the universally applicable Fick’s first law. This paper compares the predictions of these approaches for the well-studied case of a two-dimensional bubble growing in an unbounded supersaturated solution for three different levels of supersaturation. The equivalent two-dimensional simulations are run in a previously developed volume of fluid framework on OpenFOAM® [K. J. Vachaparambil and K. E. Einarsrud, Appl. Math. Model. 81, 690–710 (2020)]. The results show that the choice of an appropriate Sh correlation can provide a reasonable estimate of bubble growth. In a more universal approach, which is relevant when the flow being simulated cannot be captured by a single Sh correlation (e.g., bubble growth/coalescence and detachment) or when existing Sh correlations are not applicable, Fick’s first law can be used to compute the driving force for bubble growth, provided that the concentration boundary layer can be resolved.
url http://dx.doi.org/10.1063/5.0020210
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