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Lattice BGK kinetic model for high speed compressible flows: hydrodynamic and nonequilibrium behaviors

机译:用于高速可压缩流动的Lattice BGK动力学模型:   流体动力学和非平衡行为

摘要

We present a simple and general approach to formulate the lattice BGK modelfor high speed compressible flows. The main point consists of two parts: anappropriate discrete equilibrium distribution function (DEDF) $\mathbf{f}^{eq}$and a discrete velocity model with flexible velocity size. The DEDF is obtainedby $\mathbf{f}^{eq}=\mathbf{C}^{-1}\mathbf{M}$, where $\mathbf{M}$ is a set ofmoment of the Maxwellian distribution function, and $\mathbf{C}$ is the matrixconnecting the DEDF and the moments. The numerical components of $\mathbf{C}$are determined by the discrete velocity model. The calculation of$\mathbf{C}^{-1}$ is based on the analytic solution which is a function of theparameter controlling the sizes of discrete velocity. The choosing of discretevelocity model has a high flexibility. The specific heat ratio of the systemcan be flexible. The approach works for the one-, two- and three-dimensionalmodel constructions. As an example, we compose a new lattice BGK kinetic modelwhich works not only for recovering the Navier-Stokes equations in thecontinuum limit but also for measuring the departure of system from itsthermodynamic equilibrium. Via adjusting the sizes of the discrete velocitiesthe stably simulated Mach number can be significantly increased up to 30 oreven higher. The model is verified and validated by well-known benchmark tests.Some macroscopic behaviors of the system due to deviating from thermodynamicequilibrium around the shock wave interfaces are shown.
机译:我们提出了一种简单而通用的方法来为高速可压缩流建立晶格BGK模型。主要内容包括两部分:适当的离散平衡分布函数(DEDF)$ \ mathbf {f} ^ {eq} $和具有可变速度大小的离散速度模型。 DEDF通过$ \ mathbf {f} ^ {eq} = \ mathbf {C} ^ {-1} \ mathbf {M} $获得,其中$ \ mathbf {M} $是Maxwellian分布函数的矩集, $ \ mathbf {C} $是连接DEDF和矩的矩阵。 $ \ mathbf {C} $的数字分量由离散速度模型确定。 $ \ mathbf {C} ^ {-1} $的计算基于解析解,该解析解是控制离散速度大小的参数的函数。离散速度模型的选择具有很高的灵活性。系统的比热比可以灵活。该方法适用于一维,二维和三维模型构造。例如,我们构建了一个新的晶格BGK动力学模型,该模型不仅可用于恢复连续谱极限中的Navier-Stokes方程,而且还可用于测量系统偏离其热力学平衡的程度。通过调整离散速度的大小,可以将稳定模拟的马赫数显着提高到30甚至更高。通过众所周知的基准测试对该模型进行了验证和验证。示出了由于冲击波界面周围的热力学平衡而导致的系统的一些宏观行为。

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