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024 7 _ |2 DOI
|a 10.1103/PhysRevE.85.031601
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084 _ _ |2 WoS
|a Physics, Fluids & Plasmas
084 _ _ |2 WoS
|a Physics, Mathematical
100 1 _ |0 P:(DE-Juel1)VDB104034
|a Brener, E.A.
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245 _ _ |a Onsager approach to the one-dimensional solidification problem and its relation to the phase-field description
260 _ _ |a College Park, Md.
|b APS
|c 2012
264 _ 1 |3 online
|2 Crossref
|b American Physical Society (APS)
|c 2012-03-19
264 _ 1 |3 print
|2 Crossref
|b American Physical Society (APS)
|c 2012-03-01
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440 _ 0 |0 4924
|a Physical Review E
|v 85
|x 1539-3755
|y 3
500 _ _ |3 POF3_Assignment on 2016-02-29
500 _ _ |a We thank M. Plapp for useful discussions. We acknowledge the support of the Deutsche Forschungs-gemeinschaft under Project No. SFB 917.
520 _ _ |a We give a general phenomenological description of the steady-state 1D front propagation problem in two cases: the solidification of a pure material and the isothermal solidification of two-component dilute alloys. The solidification of a pure material is controlled by the heat transport in the bulk and the interface kinetics. The isothermal solidification of two-component alloys is controlled by the diffusion in the bulk and the interface kinetics. We find that the condition of positive-definiteness of the symmetric Onsager matrix of interface kinetic coefficients still allows an arbitrary sign of the slope of the velocity-concentration line near the solidus in the alloy problem or of the velocity-temperature line in the case of solidification of a pure material. This result offers a very simple and elegant way to describe the interesting phenomenon of a possible non-single-value behavior of velocity versus concentration that has previously been discussed by different approaches. We also discuss the relation of this Onsager approach to the thin-interface limit of the phase-field description.
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773 _ _ |a 10.1103/PhysRevE.85.031601
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