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Diffuse-interface modeling of liquid-vapor phase separation in a van der Waals fluid

机译:范德华流体中汽-液相分离的扩散界面建模

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We simulate liquid-vapor phase separation in a van der Waals fluid that is deeply quenched into the unstable range of its phase diagram. Our theoretical approach follows the diffuse-interface model, where convection induced by phase change is accounted for via a nonequilibrium (Korteweg) force expressing the tendency of the liquid-vapor system to minimize its free energy. Spinodal decomposition patterns for critical and off-critical van der Waals fluids are studied numerically, revealing the scaling laws of the characteristic length scale and composition of single-phase microdomains, together with their dependence on the Reynolds number. Unlike phase separation of viscous binary mixtures, here local equilibrium is reached almost immediately after single-phase domains start to form. In addition, as predicted by scaling laws, such domains grow in time like t(2/3). Comparison between 2D and 3D results reveals that 2D simulations capture, even quantitatively, the main features of the phenomenon.
机译:我们模拟了范德华流体中的汽-液相分离,该流体被深度淬灭到其相图的不稳定范围内。我们的理论方法遵循扩散界面模型,在该模型中,由相变引起的对流通过非平衡力(Korteweg)来解释,该力表达了液汽系统使自由能最小化的趋势。对临界和非临界范德华流体的旋节线分解模式进行了数值研究,揭示了特征长度尺度和单相微区组成的尺度定律,以及它们对雷诺数的依赖性。与粘性二元混合物的相分离不同,此处单相畴开始形成后几乎立即达到局部平衡。另外,正如缩放定律所预测的那样,此类域的时间像t(2/3)一样增长。 2D和3D结果之间的比较表明,2D模拟甚至可以定量地捕获现象的主要特征。

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