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Evaluation of Particle Resuspension and Single-layer Rates with Exposure Time and Friction Velocity for Multilayer Deposits in a Turbulent Boundary Layer

机译:湍流边界层中多层沉积物的颗粒重悬和单层速率与暴露时间和摩擦速度的评估

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The present work deals with the resuspension of small nondeformable particles from multilayer deposits in a turbulent boundary layer. A kinetic force-balance approach was adopted to model particle motion at the point of detachment, whereby intermolecular interactions were modeled by the Lennard-Jones potential. The rate of change of the number of particles was estimated for each discrete layer based on existing kinetic models. In particular, the kinetic equations of Lazaridis and Drossinos (1998), LD , and Friess and Yadigaroglu (2001), FY , were implemented and compared using lattice arranged deposits. The influence of exposure time and friction velocity was investigated through the obtained resuspension rates. It was found that the single-layer resuspension rates were substantially affected by the layer position within the deposit as well as considerably influenced by both the exposure time and the friction velocity. Moreover, the numerical results demonstrate that the LD kinetic estimates higher resuspension rates compared to the FY kinetic only for short exposures to the flow, predominantly due to a different expression for the fraction of exposed particles. In addition, the present study recognized the time dependence (i.e., a short-term vs. long-term regime) of the resuspension rate observed both experimentally (Wu et al. , 1992; Wang et al. , 2012) and by model predictions (Lazaridis and Drossinos, 1998; Friess and Yadigaroglu, 2001; Reeks and Hall, 2001) and confirmed the inverse dependence of the resuspension rate with time in long-term regime. Two regimes were also identified while evaluating the resuspension rate for a range of friction velocities, viz., a low-friction regime in which the resuspension rate increases with friction and a high-friction regime in which the opposite behaviour was observed.
机译:目前的工作是处理湍流边界层中多层沉积物中不可变形的小颗粒的重悬浮。采用了动力平衡方法来模拟脱离点的粒子运动,从而通过Lennard-Jones势来模拟分子间的相互作用。基于现有的动力学模型,估计每个离散层的颗粒数量变化率。尤其是,使用格子排列的沉积物实施并比较了Lazaridis和Drossinos(1998),LD以及Friess和Yadigaroglu(2001),FY的动力学方程。通过获得的重悬率研究了暴露时间和摩擦速度的影响。已经发现,单层重悬浮速率基本上受沉积物中层位置的影响,同时也受曝光时间和摩擦速度的影响。此外,数值结果表明,LD动力学仅在短时间暴露于流中时才比FY动力学估算出更高的重悬浮率,这主要是由于暴露颗粒的分数表达不同所致。此外,本研究还通过实验(Wu等人,1992; Wang等人,2012)和模型预测观察到了重悬率的时间依赖性(即短期与长期状态)。 (Lazaridis和Drossinos,1998; Friess和Yadigaroglu,2001; Reeks和Hall,2001)并证实了长期使用率对悬浮速率的依赖性。在评估一系列摩擦速度的重悬率时,还确定了两种状态,即低摩擦状态(其中重悬率随摩擦而增加)和高摩擦状态(其中观察到相反的行为)。

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