Rei Ogawa, Hiroki Kusudo, Takeshi Omori, Edward R. Smith, Laurent Joly, Samy Merabia, Yasutaka Yamaguchi
{"title":"Mechanical and thermodynamic routes to the liquid-liquid interfacial tension and mixing free energy by molecular dynamics","authors":"Rei Ogawa, Hiroki Kusudo, Takeshi Omori, Edward R. Smith, Laurent Joly, Samy Merabia, Yasutaka Yamaguchi","doi":"arxiv-2409.10856","DOIUrl":null,"url":null,"abstract":"In this study, we carried out equilibrium molecular dynamics (EMD)\nsimulations of the liquid-liquid interface between two different Lennard-Jones\ncomponents with varying miscibility, where we examined the relation between the\ninterfacial tension and isolation free energy using both a mechanical and\nthermodynamic approach. Using the mechanical approach, we obtained a stress\ndistribution around a quasi-one-dimensional (1D) EMD systems with a flat LL\ninterface. From the stress distribution, we calculated the liquid-liquid\ninterfacial tension based on Bakker's equation, which uses the stress\nanisotropy around the interface, and measures how it varies with miscibility.\nThe second approach uses thermodynamic integration by enforcing quasi-static\nisolation of the two liquids to calculate the free energy. This uses the same\nEMD systems as the mechanical approach, with both extended dry-surface and\nphantom-wall (PW) schemes applied. When the two components were immiscible, the\ninterfacial tension and isolation free energy were in good agreement, provided\nall kinetic and interaction contributions were included in the stress. When the\ncomponents were miscible, the values were significantly different. From the\nresult of PW for the case of completely mixed liquids, the difference was\nattributed to the additional free energy required to separate the binary\nmixture into single components against the osmotic pressure prior to the\ncomplete detachment of the two components, i.e., the free energy of mixing.","PeriodicalId":501304,"journal":{"name":"arXiv - PHYS - Chemical Physics","volume":"17 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Chemical Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.10856","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
In this study, we carried out equilibrium molecular dynamics (EMD)
simulations of the liquid-liquid interface between two different Lennard-Jones
components with varying miscibility, where we examined the relation between the
interfacial tension and isolation free energy using both a mechanical and
thermodynamic approach. Using the mechanical approach, we obtained a stress
distribution around a quasi-one-dimensional (1D) EMD systems with a flat LL
interface. From the stress distribution, we calculated the liquid-liquid
interfacial tension based on Bakker's equation, which uses the stress
anisotropy around the interface, and measures how it varies with miscibility.
The second approach uses thermodynamic integration by enforcing quasi-static
isolation of the two liquids to calculate the free energy. This uses the same
EMD systems as the mechanical approach, with both extended dry-surface and
phantom-wall (PW) schemes applied. When the two components were immiscible, the
interfacial tension and isolation free energy were in good agreement, provided
all kinetic and interaction contributions were included in the stress. When the
components were miscible, the values were significantly different. From the
result of PW for the case of completely mixed liquids, the difference was
attributed to the additional free energy required to separate the binary
mixture into single components against the osmotic pressure prior to the
complete detachment of the two components, i.e., the free energy of mixing.