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Density-amplitude formulation of the phase-field crystal model for two-phase coexistence in two and three dimensions

机译:二维和二维两相共存的相场晶体模型的密度-振幅公式

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The phase-field crystal approach describes the dynamics of the local atomic probability density on atomic length and diffusive time scales. However, the small grid spacing required to resolve the atomic length scale restricts the applicability to relatively small systems. We present a new amplitude-equation formulation that can be applied to model the evolution of a two-phase system by building upon the multiple-scale approach developed for the phase-field crystal model that explicitly incorporates a miscibility gap in the atomic density field. The new set of equations are less stiff by two orders in the spatial derivative and are found to retain acceptable accuracy even with a significantly larger grid size. Furthermore, the proposed model provides insight into the link between the phase-field-crystal model and a phase-field model in which conserved and nonconserved dynamics are coupled to describe a solid-liquid system. Models and simulation results are presented for two-dimensional hexagonal and three-dimensional body-centered cubic structures. Validation of the two-dimensional model is carried out by examining the Gibbs-Thomson effect. Simulations of growth and coarsening are performed to demonstrate the model's potential for large-scale simulations.
机译:相场晶体方法描述了原子长度和扩散时标上的局部原子概率密度的动力学。但是,解决原子长度尺度所需的小网格间距将其适用性限制在相对较小的系统上。我们提出了一种新的振幅方程公式,该公式可通过为相场晶体模型开发的多尺度方法建立模型来建模两相系统的演化,该方法在原子密度场中明确包含了可混性间隙。新的方程组在空间导数上的刚性降低了两个数量级,并且即使在较大的网格尺寸下也可以保持可接受的精度。此外,所提出的模型提供了对相场-晶体模型与相场模型之间的联系的洞察力,其中保守和非保守动力学被耦合以描述固液系统。给出了二维六边形和三维体心立方结构的模型和仿真结果。通过检查吉布斯-汤姆森效应进行二维模型的验证。进行了生长和粗化的仿真,以证明该模型在大规模仿真中的潜力。

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