稀疏两相湍流的惯性颗粒倾向性弥散  

INERTIA PARTICLE PREFERENTIAL DISPERSION IN DILUTE TWO-PHASE TURBULENT FLOWS

作　　者：王兵[1] 张会强[1] 王希麟[1] 

机构地区：[1]清华大学航天航空学院北京市3E能源重点实验室,北京100084

出　　处：《力学学报》2009年第6期821-827,共7页Chinese Journal of Theoretical and Applied Mechanics

基　　金：国家自然科学基金(50706021);高校博士点基金(20070003018)资助项目~~

摘　　要：气相采用大涡模拟、颗粒相采用拉格朗日轨道模型的方法对后台阶突扩流、充分发展槽道流和圆湍射流3种典型的稀疏气固两相流动进行了数值模拟,研究了颗粒倾向性弥散的特征和规律。研究表明颗粒的跟随性和倾向性相联系,颗粒惯性和大涡结构同时决定颗粒的倾向性分布特征。Stokes数量级为1(气相时间参考尺度取为宏观特征时间尺度)左右的颗粒,倾向性分布特征最强烈。颗粒倾向分布于低涡量(或是低脉动速度)的湍流区域。Preferential dispersion of the particles was numerically studied in three types of turbulent flows, namely, the flow over a backward-facing step, the fully developed channel flow and the round jet flow. Gas-phase was simulated by means of large eddy simulation and particle-phase was tracked by particle trajectory model. It＇s shown that inertia particles have preferential dispersion in the three turbulent flows, and the property of preferential motion of the particles is related to the particle following property. The particle preferential dispersions are determined both by particle inertia and by large eddy structures. Particles with Stokes number in the order of magnitude 1（based on the macro time-scale of fluid flow） have the strongest preferential distribution in large scale structures and they tend to accumulate in the turbulent regions with low vorticity or low fluctuating velocity.

关 键 词：颗粒倾向性分布 颗粒弥散 Stokes数 稀疏两相湍流 大涡模拟 

分 类 号：O359[理学—流体力学]