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Seeding approach to nucleation in the NVT ensemble: The case of bubble cavitation in overstretched Lennard Jones fluids

dc.contributor.authorRosales Peláez, Pablo
dc.contributor.authorSánchez Burgos, Ignacio
dc.contributor.authorValeriani, Chantal
dc.contributor.authorVega De Las Heras, Carlos
dc.contributor.authorSanz García, Eduardo Santiago
dc.date.accessioned2023-06-16T15:17:23Z
dc.date.available2023-06-16T15:17:23Z
dc.date.issued2020-02-25
dc.description©2020 American Physical Society. This work was funded by Grant No. FIS2016/78117-P of the MEC. C. Valeriani thanks financial support from FIS2016-78847-P of the MEC. The authors acknowledge the computer resources and technical assistance provided by the RES. P.R. thanks a doctoral grant from UCM.
dc.description.abstractSimulations are widely used to study nucleation in first order phase transitions due to the fact that they have access to the relevant length and time scales. However, simulations face the problem that nucleation is an activated process. Therefore, rare event simulation techniques are needed to promote the formation of the critical nucleus. The Seeding method, where the simulations are started with the nucleus already formed, has proven quite useful in efficiently providing estimates of the nucleation rate for a wide range of orders of magnitude. So far, Seeding has been employed in the NPT ensemble, where the nucleus either grows or redissolves. Thus, several trajectories have to be run in order to find the thermodynamic conditions that make the seeded nucleus critical. Moreover, the nucleus lifetime is short and the statistics for obtaining its properties is consequently poor. To deal with these shortcomings we extend the Seeding method to the NVT ensemble. We focus on the problem of bubble nucleation in a metastable Lennard Jones fluid. We show that, in the NVT ensemble, it is possible to equilibrate and stabilise critical bubbles for a long time. The nucleation rate inferred from NVT-Seeding is fully consistent with that coming from NPT-Seeding. The former is quite suitable to obtain the nucleation rate along isotherms, whereas the latter is preferable if the dependence of the rate with temperature at constant pressure is required. Care should be taken with finite size effects when using NVT-Seeding. Further work is required to extend NVT seeding to other sorts of phase transitions.
dc.description.departmentDepto. de Estructura de la Materia, Física Térmica y Electrónica
dc.description.facultyFac. de Ciencias Físicas
dc.description.refereedTRUE
dc.description.sponsorshipMinisterio de Educación y Ciencia (MEC)
dc.description.sponsorshipUniversidad Complutense de Madrid (UCM)
dc.description.statuspub
dc.eprint.idhttps://eprints.ucm.es/id/eprint/60239
dc.identifier.doi10.1103/PhysRevE.101.022611
dc.identifier.issn2470-0045
dc.identifier.officialurlhttps://doi.org/10.1103/PhysRevE.101.022611
dc.identifier.relatedurlhttps://journals.aps.org/
dc.identifier.urihttps://hdl.handle.net/20.500.14352/6200
dc.issue.number2
dc.journal.titlePhysical review E
dc.language.isoeng
dc.publisherAmerican Physical Society
dc.relation.projectIDFIS2016/78117-P; FIS2016-78847-P
dc.rights.accessRightsopen access
dc.subject.cdu539.1
dc.subject.keywordFree-energy
dc.subject.keywordHomogeneous nucleation
dc.subject.keywordGerm-formation
dc.subject.keywordNacl
dc.subject.ucmFísica nuclear
dc.subject.unesco2207 Física Atómica y Nuclear
dc.titleSeeding approach to nucleation in the NVT ensemble: The case of bubble cavitation in overstretched Lennard Jones fluids
dc.typejournal article
dc.volume.number101
dspace.entity.typePublication
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