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A comparative analysis of particle tracking in a mixer by discrete element method and positron emission particle tracking

机译:用离散元法和正电子发射粒子跟踪对混合器中粒子跟踪的对比分析

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摘要

Characterisation of particle flow using Positron Emission Particle Tracking (PEPT) is based on tracking the position of a single particle in a dynamic system. Recent developments in PEPT have facilitated tracking multiple particles aiming at improvements in data representation. Nevertheless for systems with a wide residence time distribution and/or dead zone, the conditions for getting representative data which could reflect the bulk behaviour of the powders need to be analysed and specified. In the present work, an attempt is made to simulate PEPT experiments for a paddle mixer using Discrete Element Method (DEM), with a view to investigate the effect of increasing the number of tracers on their time-averaged velocity distribution and whether it can represent the data on whole population of particles. The time averaged velocity distribution of the individual tracer particles (resembling simulated PEPT) is obtained and compared with the time averaged data on entire particle population. The DEM results indicate that for the investigated paddle mixer, it takes 251. s for one tracer to travel adequately in all the active space of the system. The instantaneous tracer velocity fluctuates around the average value obtained for all the particles, suggesting that the average tracer velocity is adequately representative of the average particle velocity in the system. The data of the PEPT experiment with one tracer with those of DEM with one tracer are in good agreement; however, DEM simulation suggests that increasing the number of tracers in the paddle mixer system does not influence the average velocity distribution. Furthermore, the velocity for all particles in the DEM shows a smooth distribution with a peak frequency of the velocity distribution that is lower than PEPT and DEM tracer. When tracking a single tracer in DEM or PEPT, it may not be detected to have zero velocity at any instant of time, whilst the data for all particles show that about 0.3% of particles are stagnant.
机译:使用正电子发射粒子跟踪(PEPT)表征粒子流的方法是基于跟踪动态系统中单个粒子的位置。 PEPT的最新发展已促进跟踪多个粒子,旨在改善数据表示。然而,对于具有宽的停留时间分布和/或死区的系统,需要分析和指定用于获得可以反映粉末的整体性能的代表性数据的条件。在当前的工作中,尝试使用离散元方法(DEM)模拟桨式混合机的PEPT实验,以研究增加示踪剂数量对其时间平均速度分布的影响及其是否可以表示有关粒子总数的数据。获得了单个示踪粒子的时间平均速度分布(类似于模拟的PEPT),并将其与整个粒子群体的时间平均数据进行了比较。 DEM结果表明,对于所研究的桨式混合器,一台示踪剂在系统的所有活动空间中充分传播都需要251秒。示踪剂的瞬时速度在所有颗粒的平均值附近波动,这表明示踪剂的平均速度足以代表系统中的平均颗粒速度。用一种示踪剂进行的PEPT实验数据与用一种示踪剂进行的DEM实验数据完全吻合;但是,DEM仿真表明,增加桨式搅拌机系统中示踪剂的数量不会影响平均速度分布。此外,DEM中所有粒子的速度都显示出平滑的分布,且速度分布的峰值频率低于PEPT和DEM示踪剂。在DEM或PEPT中跟踪单个示踪剂时,在任何时刻都可能不会检测到其速度为零,而所有粒子的数据都显示约0.3%的粒子处于停滞状态。

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