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Convective Instabilities in Two Liquid Layers

We perform linear stability calculations for horizontal fluid bilayers, taking into account both buoyancy effects and thermocapillary effects in the presence of a vertical temperature gradient. To help understand the mechanisms driving the instability, we have performed both long-wavelength and shor...

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Detalles Bibliográficos
Autores principales: McFadden, G. B., Coriell, S. R., Gurski, K. F., Cotrell, D. L.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: [Gaithersburg, MD] : U.S. Dept. of Commerce, National Institute of Standards and Technology 2007
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4656015/
https://www.ncbi.nlm.nih.gov/pubmed/27110470
http://dx.doi.org/10.6028/jres.112.020
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author McFadden, G. B.
Coriell, S. R.
Gurski, K. F.
Cotrell, D. L.
author_facet McFadden, G. B.
Coriell, S. R.
Gurski, K. F.
Cotrell, D. L.
author_sort McFadden, G. B.
collection PubMed
description We perform linear stability calculations for horizontal fluid bilayers, taking into account both buoyancy effects and thermocapillary effects in the presence of a vertical temperature gradient. To help understand the mechanisms driving the instability, we have performed both long-wavelength and short-wavelength analyses. The mechanism for the large wavelength instability is complicated, and the detailed form of the expansion is found to depend on the Crispation and Bond numbers. The system also allows a conventional Rayleigh-Taylor instability if heavier fluid overlies lighter fluid, and the long-wavelength analysis describes this case as well. In addition to the asymptotic analyses for large and small wavelengths, we have performed numerical calculations using materials parameters for a benzene-water system.
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spelling pubmed-46560152016-04-22 Convective Instabilities in Two Liquid Layers McFadden, G. B. Coriell, S. R. Gurski, K. F. Cotrell, D. L. J Res Natl Inst Stand Technol Article We perform linear stability calculations for horizontal fluid bilayers, taking into account both buoyancy effects and thermocapillary effects in the presence of a vertical temperature gradient. To help understand the mechanisms driving the instability, we have performed both long-wavelength and short-wavelength analyses. The mechanism for the large wavelength instability is complicated, and the detailed form of the expansion is found to depend on the Crispation and Bond numbers. The system also allows a conventional Rayleigh-Taylor instability if heavier fluid overlies lighter fluid, and the long-wavelength analysis describes this case as well. In addition to the asymptotic analyses for large and small wavelengths, we have performed numerical calculations using materials parameters for a benzene-water system. [Gaithersburg, MD] : U.S. Dept. of Commerce, National Institute of Standards and Technology 2007 2007-10-01 /pmc/articles/PMC4656015/ /pubmed/27110470 http://dx.doi.org/10.6028/jres.112.020 Text en https://creativecommons.org/publicdomain/zero/1.0/ The Journal of Research of the National Institute of Standards and Technology is a publication of the U.S. Government. The papers are in the public domain and are not subject to copyright in the United States. Articles from J Res may contain photographs or illustrations copyrighted by other commercial organizations or individuals that may not be used without obtaining prior approval from the holder of the copyright.
spellingShingle Article
McFadden, G. B.
Coriell, S. R.
Gurski, K. F.
Cotrell, D. L.
Convective Instabilities in Two Liquid Layers
title Convective Instabilities in Two Liquid Layers
title_full Convective Instabilities in Two Liquid Layers
title_fullStr Convective Instabilities in Two Liquid Layers
title_full_unstemmed Convective Instabilities in Two Liquid Layers
title_short Convective Instabilities in Two Liquid Layers
title_sort convective instabilities in two liquid layers
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4656015/
https://www.ncbi.nlm.nih.gov/pubmed/27110470
http://dx.doi.org/10.6028/jres.112.020
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