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Negative pressure characteristics of an evaporating meniscus at nanoscale

This study aims at understanding the characteristics of negative liquid pressures at the nanoscale using molecular dynamics simulation. A nano-meniscus is formed by placing liquid argon on a platinum wall between two nano-channels filled with the same liquid. Evaporation is simulated in the meniscus...

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Detalles Bibliográficos
Autores principales: Maroo, Shalabh C, Chung, JN
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Springer 2011
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3212220/
https://www.ncbi.nlm.nih.gov/pubmed/21711621
http://dx.doi.org/10.1186/1556-276X-6-72
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author Maroo, Shalabh C
Chung, JN
author_facet Maroo, Shalabh C
Chung, JN
author_sort Maroo, Shalabh C
collection PubMed
description This study aims at understanding the characteristics of negative liquid pressures at the nanoscale using molecular dynamics simulation. A nano-meniscus is formed by placing liquid argon on a platinum wall between two nano-channels filled with the same liquid. Evaporation is simulated in the meniscus by increasing the temperature of the platinum wall for two different cases. Non-evaporating films are obtained at the center of the meniscus. The liquid film in the non-evaporating and adjacent regions is found to be under high absolute negative pressures. Cavitation cannot occur in these regions as the capillary height is smaller than the critical cavitation radius. Factors which determine the critical film thickness for rupture are discussed. Thus, high negative liquid pressures can be stable at the nanoscale, and utilized to create passive pumping devices as well as significantly enhance heat transfer rates.
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spelling pubmed-32122202011-11-09 Negative pressure characteristics of an evaporating meniscus at nanoscale Maroo, Shalabh C Chung, JN Nanoscale Res Lett Nano Express This study aims at understanding the characteristics of negative liquid pressures at the nanoscale using molecular dynamics simulation. A nano-meniscus is formed by placing liquid argon on a platinum wall between two nano-channels filled with the same liquid. Evaporation is simulated in the meniscus by increasing the temperature of the platinum wall for two different cases. Non-evaporating films are obtained at the center of the meniscus. The liquid film in the non-evaporating and adjacent regions is found to be under high absolute negative pressures. Cavitation cannot occur in these regions as the capillary height is smaller than the critical cavitation radius. Factors which determine the critical film thickness for rupture are discussed. Thus, high negative liquid pressures can be stable at the nanoscale, and utilized to create passive pumping devices as well as significantly enhance heat transfer rates. Springer 2011-01-12 /pmc/articles/PMC3212220/ /pubmed/21711621 http://dx.doi.org/10.1186/1556-276X-6-72 Text en Copyright ©2011 Maroo and Chung; licensee Springer. http://creativecommons.org/licenses/by/2.0 This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
spellingShingle Nano Express
Maroo, Shalabh C
Chung, JN
Negative pressure characteristics of an evaporating meniscus at nanoscale
title Negative pressure characteristics of an evaporating meniscus at nanoscale
title_full Negative pressure characteristics of an evaporating meniscus at nanoscale
title_fullStr Negative pressure characteristics of an evaporating meniscus at nanoscale
title_full_unstemmed Negative pressure characteristics of an evaporating meniscus at nanoscale
title_short Negative pressure characteristics of an evaporating meniscus at nanoscale
title_sort negative pressure characteristics of an evaporating meniscus at nanoscale
topic Nano Express
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3212220/
https://www.ncbi.nlm.nih.gov/pubmed/21711621
http://dx.doi.org/10.1186/1556-276X-6-72
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