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Stochastic modeling of fluid velocity seen by heavy particles for two-phase LES of non-homogeneous and anisotropic turbulent flows

机译:两相叶片非均相和各向异性湍流术的重型粒子流体速度的随机塑造

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The neglect of the effects of sub-filter scale velocities often remains a source of error in LES predictions of particle dispersion and deposition. Indeed, sub-filter fluctuations should be expected to be more significant for particles with smaller relaxation times compared to the LES-resolved turbulence time scales. In this work, a stochastic diffusion process is used to include the sub-filter scale transport when tracking a dilute suspension of heavy particles (glass beads in air with different Stokes' numbers, namely 0.022 and 2.8) in a high Reynolds number, equilibrium turbulent shear flow (Re_τ = 2,200 based on the friction velocity and the pipe diameter). A Langevin-type equation is proposed to model the Lagrangian fluid velocity seen by solid particles, taking into account inertia and cross-trajectory effects. LES predictions are compared to RANS results and experimental observations. It is shown that the RANS approach is unable to predict particle dispersion statistics as accurately as LES does, especially for inertial particles characterized by a Stokes number smaller than one. For particles with Stokes number higher than one, both LES and RANS predictions compare reasonably well with the experimental results. More importantly, the use of a stochastic approach to model the sub-filter scale fluctuations has proven crucial for results concerning the small-Stokes-number particles. The model requires additional validation for non-equilibrium turbulent flows.
机译:忽略子过滤量速度速度的影响通常仍然是粒子分散和沉积的LES预测中的误差源。实际上,与LES分辨的湍流时间尺度相比,粒子过滤器波动应与较小弛豫时间的颗粒更加重要。在这项工作中,随机扩散过程用于在高雷诺数中跟踪重型颗粒的稀释悬浮液(在空气中的玻璃珠,即0.022和2.8)中的稀释悬浮液中,在高雷诺数,平衡湍流剪切流动(Re_τ= 2,200基于摩擦速度和管道直径)。提出了一种LangeVin型方程来模拟固体颗粒的拉格朗日流体速度,考虑到惯性和交叉轨迹效果。将LES预测与RAN结果和实验观察进行了比较。结果表明,随着LES的表现,RAN方法不能像LES一样准确地预测粒子分散统计数据,特别是对于以小于1的斯托克斯数而表征的惯性粒子。对于具有高于1的斯托克斯号的粒子,LES和RANS预测都与实验结果相比相当良好。更重要的是,使用随机方法来模拟模型的子滤光尺度波动已经证明是关于小型斯托克号粒子的结果。该模型需要对非平衡湍流流动的额外验证。

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