Propagating phase interface with intermediate interfacial phase: Phase field approach

dc.contributor.author Momeni, Kasra
dc.contributor.author Levitas, Valery
dc.contributor.author Levitas, Valery
dc.contributor.department Aerospace Engineering
dc.date 2018-02-14T01:36:22.000
dc.date.accessioned 2020-06-29T22:45:58Z
dc.date.available 2020-06-29T22:45:58Z
dc.date.copyright Wed Jan 01 00:00:00 UTC 2014
dc.date.embargo 8000-01-01
dc.date.issued 2014-01-01
dc.description.abstract <p>An advanced three-phase phase field approach (PFA) is suggested for a nonequilibrium phase interface that contains an intermediate phase, in particular, a solid-solid interface with a nanometer-sized intermediate melt (IM). A thermodynamic potential in the polar order parameters is developed that satisfies all thermodynamic equilibrium and stability conditions. The special form of the gradient energy allowed us to include the interaction of two solid-melt interfaces via an intermediate melt and obtain a well-posed problem and mesh-independent solutions. It is proved that for stationary 1D solutions to two Ginzburg-Landau equations for three phases, the local energy at each point is equal to the gradient energy. Simulations are performed for β ↔ δ phase transformations (PTs) via IM in an HMX energetic material. The obtained energy IM width dependence is described by generalized force-balance models for short- and long-range interaction forces between interfaces but not far from the melting temperature. A force-balance model is developed that describes phase field results even 100 K below the melting temperature. The effects of the ratios of width and energies of solid-solid and solid-melt interfaces, temperature, and the parameter characterizing interaction of two solid-melt interfaces, on the structure, width, energy of the IM and interface velocity are determined by finite element method. Depending on parameters, the IM may appear by continuous or discontinuous barrierless disordering or via critical nucleus due to thermal fluctuations. The IM may appear during heating and persist during cooling at temperatures well belowthan it follows from sharp-interface approach.On the other hand, for some parameters when IM is expected, it does not form, producing an IM-free gap. The developed PFA represents a quite general three-phase model and can be extended to other physical phenomena, such as martensitic PTs, surface-induced premelting and PTs, premelting/disordering at grain boundaries, and developing corresponding interfacial phase diagrams.</p>
dc.description.comments <p><p>This article is from <em>Physical Review B</em>89 (2014): 184102, doi:<a href="http://dx.doi.org/10.1103/PhysRevB.89.184102" target="_blank">10.1103/PhysRevB.89.184102</a>Posted with permission.</p></p>
dc.format.mimetype application/pdf
dc.identifier archive/lib.dr.iastate.edu/aere_pubs/44/
dc.identifier.articleid 1040
dc.identifier.contextkey 5662237
dc.identifier.s3bucket isulib-bepress-aws-west
dc.identifier.submissionpath aere_pubs/44
dc.identifier.uri https://dr.lib.iastate.edu/handle/20.500.12876/2044
dc.language.iso en
dc.source.bitstream archive/lib.dr.iastate.edu/aere_pubs/44/2014_LevitasVI_PropagatingPhaseInterface.pdf|||Sat Jan 15 00:17:12 UTC 2022
dc.source.uri 10.1103/PhysRevB.89.184102
dc.subject.disciplines Aerospace Engineering
dc.subject.disciplines Materials Science and Engineering
dc.subject.disciplines Mechanical Engineering
dc.title Propagating phase interface with intermediate interfacial phase: Phase field approach
dc.type article
dc.type.genre article
dspace.entity.type Publication
relation.isAuthorOfPublication 850871e3-115a-428e-82cc-cbfafef5cf66
relation.isOrgUnitOfPublication 047b23ca-7bd7-4194-b084-c4181d33d95d
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