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首页> 外文期刊>Journal of Computational Physics >Coarse- and fine-grid numerical behavior of MRT/TRT lattice-Boltzmann schemes in regular and random sphere packings
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Coarse- and fine-grid numerical behavior of MRT/TRT lattice-Boltzmann schemes in regular and random sphere packings

机译:MRT / TRT格-玻尔兹曼格式在规则和随机球体填充中的粗网格和细网格数值行为

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We analyze the intrinsic impact of free-tunable combinations of the relaxation rates controlling viscosity-independent accuracy of the multiple-relaxation-times (MRT) lattice-Boltzmann models. Preserving all MRT degrees of freedom, we formulate the parametrization conditions which enable the MRT schemes to provide viscosity-independent truncation errors for steady state solutions, and support them with the second-and third-order accurate ("linear" and "parabolic", respectively) boundary schemes. The parabolic schemes demonstrate the advanced accuracy with weak dependency on the relaxation rates, as confirmed by the simulations with the D3Q15 model in three regular arrays (SC, BCC, FCC) of touching spheres. Yet, the low-order, bounce-back boundary rule remains appealing for pore-scale simulations where the precise distance to the boundaries is undetermined. However, the effective accuracy of the bounce-back crucially depends on the free-tunable combinations of the relaxation rates. We find that the combinations of the kinematic viscosity rate with the available "ghost" antisymmetric collision mode rates mainly impact the accuracy of the bounce-back scheme. As the first step, we reduce them to the one combination (presented by so-called "magic" parameter Lambda in the frame of the two-relaxation-times (TRT) model), and study its impact on the accuracy of the drag force/permeability computations with the D3Q19 velocity set in two different, dense, random packings of 8000 spheres each. We also run the simulations in the regular (BCC and FCC) packings of the same porosity for the broad range of the discretization resolutions, ranging from 5 to 750 lattice nodes per sphere diameter. A special attention is given to the discretization procedure resulting in significantly reduced scatter of the data obtained at low resolutions. The results reveal the identical.-dependency versus the discretization resolution in all four packings, regular and random. While very small Lambda values overestimate the drag measurements several-fold on the coarse grids, Lambda > 1 may overestimate the permeability at the same extent. In low resolution region we provide practical guidelines, extending previously known solutions for the straight/diagonal Poiseuille flow. Analysis of the high-resolution region reveals the collapse of the solutions obtained with all the considered Lambda values with the average rate of -1.3, followed by their common, smooth, first-order convergence with the rate of -1.0 as the best, towards the reference solutions provided by the "parabolic" schemes. High-quality power-law fits estimate that the bounce-back would reach their accuracy (obtained at about 200 nodes per sphere) for two-order magnitude higher grid resolution. (C) 2014 Elsevier Inc. All rights reserved.
机译:我们分析松弛率的自由可调组合的内在影响,该松弛率控制多重弛豫时间(MRT)晶格-玻尔兹曼模型的粘度无关精度。在保留所有MRT自由度的前提下,我们制定了参数化条件,使MRT方案能够为稳态溶液提供与粘度无关的截断误差,并以二阶和三阶精度(“线性”和“抛物线”,分别)边界方案。 D3Q15模型在三个接触球体的常规阵列(SC,BCC,FCC)中的模拟证实了这种抛物线方案显示了对松弛率的弱​​依赖性的先进精度。然而,低阶反弹边界法则仍然适用于尚未确定到边界的精确距离的孔隙尺度模拟。但是,反弹的有效精度关键取决于松弛率的自由可调组合。我们发现运动粘度速率与可用的“重影”反对称碰撞模式速率的组合主要影响回弹方案的准确性。第一步,我们将它们简化为一个组合(在两个松弛时间(TRT)模型的框架中由所谓的“魔术”参数Lambda表示),并研究其对拖曳力精度的影响D3Q19速度集在两个不同的,密集的,随机填充的,每个8000个球体中进行渗透率计算。我们还对孔隙率相同的常规(BCC和FCC)填料进行了模拟,以实现宽范围的离散化分辨率,每个球体直径范围为5到750个晶格节点。特别注意离散化过程,该过程可显着减少以低分辨率获得的数据的分散性。结果表明,在所有四个填充中,规则填充和随机填充都具有相同的依赖性和离散化分辨率。尽管非常小的Lambda值会高估粗网格上的阻力测量值几倍,但Lambda> 1可能会在相同程度上高估渗透率。在低分辨率区域中,我们提供了实用指南,扩展了先前已知的直线/对角Poiseuille流解决方案。对高分辨率区域的分析显示,所有考虑的Lambda值均以-1.3的比率获得的解的崩溃,然后以-1.0为最佳的比率进行共同,平滑,一阶收敛,朝着“抛物线”方案提供的参考解决方案。高质量幂律拟合估计,对于更高的网格分辨率,反跳将达到其精度(每个球体约200个节点)。 (C)2014 Elsevier Inc.保留所有权利。

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