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Three-dimensional discrete-velocity BGK model for the incompressible Navier-Stokes equations

机译:不可压缩Navier-Stokes方程的三维离散速度BGK模型

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摘要

The lattice Boltzmann method (LBM) has been widely used for the simulations of the incompressible Navier-Stokes (NS) equations. The finite difference Boltzmann method (FDBM) in which the discrete-velocity Boltzmann equation is solved instead of the lattice Boltzmann equation has also been applied as an alternative method for simulating the incompressible flows. The particle velocities of the FDBM can be selected independently from the lattice configuration. In this paper, taking account of this advantage, we present the discrete velocity Boltzmann equation that has a minimum set of the particle velocities with the lattice Bharnagar-Gross-Krook (BGK) model for the three-dimensional incompressible NS equations. To recover incompressible NS equations, tensors of the particle velocities have to be isotropic up to the fifth rank. Thus, we propose to apply the icosahedral vectors that have 13 degrees of freedom to the particle velocity distributions. Validity of the proposed model (D3Q13BGK) is confirmed by numerical simulations of the shear-wave decay problem and the Taylor-Green vortex problem. With respect to numerical accuracy, computational efficiency and numerical stability, we compare the proposed model with the conventional lattice BGK models (D3Q15, D3Q19 and D3Q27) and the multiple-relaxation-time (MRT) model (D3Q13MRT) that has the same degrees of freedom as our proposal. The comparisons show that the compressibility error of the proposed model is approximately double that of the conventional lattice BGK models, but the computational efficiency of the proposed model is superior to that of the others. The linear stability of the proposed model is also superior to that of the lattice BGK models. However, in non-linear simulations, the proposed model tends to be less stable than the others.
机译:格子玻尔兹曼方法(LBM)已被广泛用于不可压缩的Navier-Stokes(NS)方程的模拟。求解离散速度Boltzmann方程而不是晶格Boltzmann方程的有限差分Boltzmann方法(FDBM)也已用作模拟不可压缩流的替代方法。 FDBM的粒子速度可以独立于晶格配置进行选择。在本文中,考虑到这一优势,我们使用三维不可压缩NS方程的格子Bharnagar-Gross-Krook(BGK)模型,提出了具有最小粒子速度集的离散速度Boltzmann方程。为了恢复不可压缩的NS方程,粒子速度的张量必须是各向同性的,直到第五级。因此,我们建议将具有13个自由度的二十面体矢量应用于粒子速度分布。剪切波衰减问题和泰勒-格林涡旋问题的数值模拟证实了所提出模型(D3Q13BGK)的有效性。在数值精度,计算效率和数值稳定性方面,我们将提出的模型与传统的点阵BGK模型(D3Q15,D3Q19和D3Q27)和多次松弛时间(MRT)模型(D3Q13MRT)进行了比较。自由是我们的建议。比较表明,该模型的可压缩性误差约为传统点阵BGK模型的两倍,但是该模型的计算效率优于其他模型。所提出模型的线性稳定性也优于晶格BGK模型。然而,在非线性仿真中,所提出的模型比其他模型更不稳定。

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