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A cascaded phase-field lattice Boltzmann model for the simulation of incompressible, immiscible fluids with high density contrast

机译:级联相场晶格玻尔兹曼模型,用于模拟具有高密度对比的不可压缩,不互溶的流体

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In this work, a conservative phase-field model for the simulation of immiscible multiphase flows is developed using an incompressible, velocity-based, cascaded lattice Boltzmann method (CLBM). Extensions are made to the lattice Boltzmann (LB) equations for interface tracking and incompressible hydrodynamics, proposed by Fakhari et al. [1], by performing relaxation operations in central moment space. This was motivated by the work of Fei et al. [2,3], where promising results from such a transformation were observed. The relaxation of central moments is defined in a reference frame moving with the fluid, while the existing multiple-relaxation time [4,5] scheme performs collision in a fixed frame of reference. Moreover, the derivations make use of continuous, Maxwellian distribution functions. As a result, the CLBM enhances the Galilean invariance and stability of the method when high lattice Mach numbers are evident. The cascaded scheme has been previously used in the literature to simulate multiphase flows based on the pseudo-potential model, where it allowed for high density and viscosity contrasts to be captured [6,7]. Here, the CLBM is implemented within the phase-field framework and is verified through the analysis of a layered Poiseuille flow. The performance of the CLBM is then investigated in terms of spurious currents, Galilean invariance and computational efficiency. Finally, the work of Fakhari et al. [1] is extended by validating the model's ability to capture the relation between surface tension and the rise velocity of a planar Taylor bubble, in both stagnant and flowing fluids. New counter-current results indicate that the rise velocity model of Ha-Ngoc and Fabre [8] also applies in this regime. (C) 2019 Elsevier Ltd. All rights reserved.
机译:在这项工作中,使用不可压缩的基于速度的级联格子玻尔兹曼方法(CLBM),开发了用于模拟不混溶多相流的保守相场模型。由Fakhari等人提出的对界面跟踪和不可压缩流体动力学的格子Boltzmann(LB)方程进行了扩展。 [1],通过在中心矩空间中执行松弛操作。这是由Fei等人的工作激发的。 [2,3],其中观察到了这种转化的有希望的结果。中心矩的松弛在随流体移动的参考系中定义,而现有的多重松弛时间[4,5]方案在固定的参考系中执行碰撞。此外,推导使用连续的麦克斯韦分布函数。结果,当高晶格马赫数明显时,CLBM增强了方法的伽利略不变性和稳定性。级联方案先前已在文献中用于基于伪势模型来模拟多相流,在该模型中,可以捕获高密度和高粘度对比[6,7]。在这里,CLBM是在相场框架内实现的,并通过对分层Poiseuille流的分析进行了验证。然后根据杂散电流,伽利略不变性和计算效率来研究CLBM的性能。最后,Fakhari等人的工作。通过验证模型捕获滞留和流动流体中表面张力与平面泰勒气泡上升速度之间关系的能力,可以扩展[1]。新的逆流结果表明,Ha-Ngoc和Fabre [8]的上升速度模型也适用于这种情况。 (C)2019 Elsevier Ltd.保留所有权利。

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