论文标题
晶格Boltzmann模拟捕获了软流晶体的多尺理物理
Lattice Boltzmann simulations capture the multiscale physics of soft flowing crystals
论文作者
论文摘要
对软流量材料的潜在物理学的研究在很大程度上取决于数值模拟,这是由于理事方程的复杂结构反映了在空间和时间上以广泛不同尺度作用的并发机制的竞争。全面的计算建模仍然是一个巨大的挑战,因为它在空间中同时处理六个或更多的空间数十年,并且时间是时间的两倍。通过实施中尺度的超分子力量,旨在以全图描述的计算成本的一小部分捕获基本物理,通常可以提供一种可行的策略来大大减轻此问题。 在这里,我们回顾了晶格玻尔兹曼中尺度方法的最新进展,用于软流动材料,包括在动态界面之间的近接触相互作用(NCI),因为它们以高包装软体数软流动晶体发生。 The method proves capable of capturing several aspects of the rheology of soft flowing crystals, namely, i) a 3/2 power-law dependence of the dispersed phase flow rate on the applied pressure gradient, ii) the structural transition between an ex-two and ex-one (bamboo) configurations with the associated drop of the flow rate, iii) the onset of interfacial waves once NCI is sufficiently intense.
The study of the underlying physics of soft flowing materials depends heavily on numerical simulations, due to the complex structure of the governing equations reflecting the competition of concurrent mechanisms acting at widely disparate scales in space and time. A full-scale computational modelling remains a formidable challenge since it amounts to simultaneously handle six or more spatial decades in space and twice as many in time. Coarse-grained methods often provide a viable strategy to significantly mitigate this issue, through the implementation of mesoscale supramolecular forces designed to capture the essential physics at a fraction of the computational cost of a full-detail description. Here, we review some recent advances in the design of a lattice Boltzmann mesoscale approach for soft flowing materials, inclusive of near-contact interactions (NCI) between dynamic interfaces, as they occur in high packing-fraction soft flowing crystals. The method proves capable of capturing several aspects of the rheology of soft flowing crystals, namely, i) a 3/2 power-law dependence of the dispersed phase flow rate on the applied pressure gradient, ii) the structural transition between an ex-two and ex-one (bamboo) configurations with the associated drop of the flow rate, iii) the onset of interfacial waves once NCI is sufficiently intense.