4.5 Article

Kinetics of solid-liquid interface motion in molecular dynamics and phase-field models: crystallization of chromium and silicon

出版社

ROYAL SOC
DOI: 10.1098/rsta.2020.0320

关键词

kinetics of crystallization; solid-liquid interface; molecular dynamics; phase-field model

资金

  1. U.S. Department of Energy, Office of Science, Basic Energy Sciences [DE-SC0019191]
  2. German Science Foundation (DFG-Deutsche Forschungsgemeinschaft) [GA 1142/11-1]
  3. U.S. National Science Foundation through the Extreme Science and Engineering Discovery Environment [TG-DMR110090]
  4. U.S. Department of Energy (DOE) [DE-SC0019191] Funding Source: U.S. Department of Energy (DOE)

向作者/读者索取更多资源

The results from molecular dynamics (MD) simulations demonstrate a complex temperature dependence of the crystal-liquid interface velocity during crystallization, with an initial increase at moderate undercooling followed by a gradual decrease at deeper levels of undercooling. Existing theoretical models fail to fully describe the MD results, but using the hodograph equation can provide a better prediction across the entire temperature range.
The results of molecular dynamics (MD) simulations of the crystallization process in one-component materials and solid solution alloys reveal a complex temperature dependence of the velocity of the crystal-liquid interface featuring an increase up to a maximum at 10-30% undercooling below the equilibrium melting temperature followed by a gradual decrease of the velocity at deeper levels of undercooling. At the qualitative level, such non-monotonous behaviour of the crystallization front velocity is consistent with the diffusion-controlled crystallization process described by the Wilson-Frenkel model, where the almost linear increase of the interface velocity in the vicinity of melting temperature is defined by the growth of the thermodynamic driving force for the phase transformation, while the decrease in atomic mobility with further increase of the undercooling drives the velocity through the maximum and into a gradual decrease at lower temperatures. At the quantitative level, however, the diffusional model fails to describe the results of MD simulations in the whole range of temperatures with a single set of parameters for some of the model materials. The limited ability of the existing theoretical models to adequately describe the MD results is illustrated in the present work for two materials, chromium and silicon. It is also demonstrated that the MD results can be well described by the solution following from the hodograph equation, previously found from the kinetic phase-field model (kinetic PFM) in the sharp interface limit. The ability of the hodograph equation to describe the predictions of MD simulation in the whole range of temperatures is related to the introduction of slow (phase field) and fast (gradient flow) variables into the original kinetic PFM from which the hodograph equation is obtained. The slow phase-field variable is responsible for the description of data at small undercoolings and the fast gradient flow variable accounts for local non-equilibrium effects at high undercoolings. The introduction of these two types of variables makes the solution of the hodograph equation sufficiently flexible for a reliable description of all nonlinearities of the kinetic curves predicted in MD simulations of Cr and Si. This article is part of the theme issue 'Transport phenomena in complex systems (part 1)'.

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