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首页> 外文期刊>Powder Technology: An International Journal on the Science and Technology of Wet and Dry Particulate Systems >Relative importance of the lift force on heavy particles due to turbulence driven secondary flows
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Relative importance of the lift force on heavy particles due to turbulence driven secondary flows

机译:湍流驱动的二次流引起的重粒子上的提升力的相对重要性

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摘要

Saffman lift forces on dense particles due to gradients in both streamwise and cross-stream velocities in a downward,fully developed turbulent square duct flow at Re_(perpendicular)=360 are studied using large eddy simulations.Volume fraction of the dispersed phase is low enough(<=10~(-5))that the one-way coupling approach is reasonable,i.e.,two-way coupling and particle-particle collisions are not considered.Eulerian and Lagrangian approaches are used to treat the continuous and dispersed phases,respectively.Subgrid stresses are modeled with the dynamic subgrid kinetic energy model of Kim and Menon [W.W.Kim and S.Menon.Application of the localized dynamic subgrid-scale model to turbulent wall-bounded flows,AIAA 97-0210,1997.].The particle equation of motion includes drag,lift forces due to both the streamwise and cross-stream velocity gradients,gravity,and is integrated using the fourth-order accurate Runge-Kutta scheme.Dependence of particle drag and lift forces on duct cross-sectional location and particle response time is demonstrated using the mean value contours and probability density functions(PDFs)of particle forces.It is shown that the streamwise component of the mean drag force experienced by particles of all response times is a deceleration force,i.e.on average,fluid streamwise velocity lags the particle streamwise velocity.Secondly,the two wall-normal(or lateral)components of the mean drag force are oriented such that the particles experience a net mean force toward the duct corners.PDFs of particle drag force components show that smaller response time particles experience a wider range of drag force about the mean value,as compared to the more inertial particles.Contours of mean wall-normal lift forces due to streamwise velocity gradients show that this force predominantly acts toward the duct walls and that the maximum lift force occurs close to the walls.PDFs of lift force due to streamwise velocity gradients show that the range of fluctuations increases with particle response time,but the dependence on particle response time is weaker compared to drag force.Lift forces due to cross-stream velocity gradients are at least an order of magnitude smaller than lift forces due to streamwise velocity gradients and are found to decrease in their range of fluctuations with particle response time.It is demonstrated that lift forces due to secondary flow velocity gradients are not as important as those due to streamwise velocity gradients in a square duct flow.
机译:在大涡模拟下,研究了向下流动(在垂直方向)= 360时充分发展的湍流方管流中由于顺流和横流速度梯度引起的萨夫曼升力对致密颗粒的影响。分散相的体积分数足够低(<= 10〜(-5))认为单向耦合是合理的,即不考虑双向耦合和粒子间碰撞。欧拉和拉格朗日方法分别用于处理连续相和分散相用金和梅农的动态子网格动能模型[WWKim和S.Menon。局部动态子网格规模模型在湍流壁面流动中的应用,AIAA 97-0210,1997。]。质点运动方程包括阻力,由流向和横流速度梯度引起的升力,重力,并使用四阶精确的Runge-Kutta方案进行积分。质点阻力和升力对管道横截​​面的依赖性利用粒子力的均值轮廓线和概率密度函数(PDFs)来证明粒子的位置和响应时间。结果表明,在所有响应时间下,粒子所受到的平均阻力的流向分量是一个减速力,即其次,平均阻力的两个壁法向分量(或横向分量)的方向是使粒子承受朝向管道角的净平均力。表明与较小的惯性粒子相比,响应时间更短的粒子承受的拉力范围更广,均值范围更大。流向速度梯度导致的平均壁法向提升力的轮廓表明,该力主要作用于管道壁和最大的升力发生在靠近壁的地方。由于沿流速度梯度的升力,PDF文件显示波动幅度增加了。与颗粒响应时间有关,但与阻力相比,对颗粒响应时间的依赖性更弱。横流速度梯度引起的提升力比流向速度梯度引起的提升力至少小一个数量级,并且发现减小结果表明,由二次流速梯度引起的升力不如方管流中沿流速度梯度引起的升力重要。

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