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首页> 外文期刊>Multiscale modeling & simulation >ON THE EULERIAN LARGE EDDY SIMULATION OF DISPERSE PHASE FLOWS: AN ASYMPTOTIC PRESERVING SCHEME FOR SMALL STOKES NUMBER FLOWS
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ON THE EULERIAN LARGE EDDY SIMULATION OF DISPERSE PHASE FLOWS: AN ASYMPTOTIC PRESERVING SCHEME FOR SMALL STOKES NUMBER FLOWS

机译:离散相流的EULERIAN大涡模拟:小Stokes数流的渐近保留格式

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In the present work, the Eulerian large eddy simulation (LES) of dilute disperse phase flows is investigated. By highlighting the main advantages and drawbacks of the available approaches in the literature, a choice is made in terms of modeling: a Fokker-Planck-like filtered kinetic equation proposed by Zaichik, Simonin, and Alipchenkov [L. I. Zaichik, O. Simonin, and V. M. Alipchenkov, J. Turbul., 10 (2009), N4] and a kinetic-based moment method based on a Gaussian closure for the number density function proposed by Vie, Doisneau, and Massot [A. Vie, F. Doisneau, and M. Massot, Comm. Comput. Phys., 17 (2015), pp. 1-46]. The resulting Euler-like system of equations is able to reproduce the dynamics of particles for small to moderate Stokes number flows, given a LES model for the gaseous phase, and is representative of the generic difficulties of such models. Indeed, it encounters strong constraints in terms of numerics in the small Stokes number limit, which can lead to a degeneracy of the accuracy of standard numerical methods. These constraints are (1) as the resulting sound speed is inversely proportional to the Stokes number, it is highly CFL constraining, and (2) the system tends to an advection-diffusion limit equation on the number density that has to be properly approximated by the designed scheme used for the whole range of Stokes numbers. Then, the present work proposes a numerical scheme that is able to handle both. Relying on the ideas introduced in a different context by Chalons, Girardin, and Kokh [C. Chalons, M. Girardin, and S. Kokh, SIAM J. Sci. Comput., 35 (2013), pp. A2874-A2902], a Lagrange projection, a relaxation formulation, and a Harten-Lax-van Leer-Contact scheme with source terms, we extend the approach to a singular flux as well as properly handle the energy equation. The final scheme is proven to be asymptotic-preserving on one-dimensional cases comparing to either converged or analytical solutions and can easily be extended to multidimensional configurations, thus setting the path for realistic applications.
机译:在目前的工作中,研究了稀疏分散相流的欧拉大涡模拟(LES)。通过突出文献中可用方法的主要优缺点,在建模方面进行了选择:Zaichik,Simonin和Alipchenkov提出的类似Fokker-Planck的滤波动力学方程。 [I. Zaichik,O. Simonin,and VM Alipchenkov,J. Turbul。,10(2009),N4]和基于高斯闭合的动力学矩量方法,由Vie,Doisneau和Massot提出[一种。 Vie,F。Doisneau和M. Massot,Comm。计算物理。17(2015),pp.1-46]。给定气相LES模型,所得的类欧拉方程组能够针对小到中等斯托克斯数流再现粒子的动力学,并且代表了此类模型的一般困难。实际上,它在较小的Stokes数限制内在数值方面遇到了严格的约束,这可能导致标准数值方法的准确性下降。这些约束是(1)由于最终的声速与斯托克斯数成反比,因此对CFL的约束很大,并且(2)系统趋向于对流扩散极限方程,该方程必须适当地近似为用于整个斯托克斯数范围的设计方案。然后,本工作提出了一种能够同时处理这两种情况的数值方案。依靠Chalons,Girardin和Kokh [C. Chalons,M。Girardin和S. Kokh,SIAM J. Sci。 [Comput。,35(2013),pp。A2874-A2902],Lagrange投影,松弛公式以及具有源项的Harten-Lax-van Leer-Contact方案,我们将方法扩展到奇异通量处理能量方程。与收敛解或解析解相比,最终方案在一维情况下被证明是渐近保持的,并且可以轻松地扩展到多维配置,从而为实际应用设置了路径。

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