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The Structure of Agglomerates Consisting of Polydisperse Particles

机译:由多分散颗粒组成的团聚体的结构

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摘要

Agglomeration is encountered in many natural or industrial processes, like growth of aerosol particles in the atmosphere and during material synthesis or even flocculation of suspensions, granulation, crystallization, and with colloidal particle processing. These particles collide by different mechanisms and stick together forming irregular or fractal-like agglomerates. Typically, the structure of these agglomerates is characterized with the fractal dimension, Df , and pre-exponential factor, kn , of simulated agglomerates of monodisperse primary particles (PP) for ballistic or diffusion-limited particle-cluster and cluster-cluster collision mechanisms. Here, the effect of PP polydispersity on Df and kn is investigated with agglomerates consisting of 16-1024 PP with closely controlled size distribution (geometric standard deviation, σg = 1-3). These simulations are in excellent agreement with the classic structure (Df and kn ) of agglomerates consisting of monodisperse PPs made by four different collision mechanisms as well as with agglomerates of bi-, tridisperse, and normally distributed PPs. Broadening the PP size distribution of agglomerates decreases monotonically their Df , and for sufficiently broad PP distributions (σg > 2.5) the Df reaches about 1.5 and kn about 1 regardless of the collision mechanism. Furthermore, with increasing PP polydispersity, the corresponding projected area exponent, Dα , and pre-exponential factor, ka , decrease monotonically from their standard values for agglomerates with monodisperse PPs. So Df as well as Dα and ka can be an indication for PP polydispersity in mass mobility and light scattering measurements if the dominant agglomeration mechanism is known, like diffusion-limited and/or ballistic cluster-cluster coagulation in aerosols.
机译:在许多自然或工业过程中都会遇到结块,例如大气中气溶胶颗粒的生长以及材料合成过程中,甚至悬浮液的絮凝,造粒,结晶以及胶体颗粒处理。这些颗粒通过不同的机理碰撞并粘在一起,形成不规则的或分形的附聚物。通常,这些团聚体的结构以单分散初级颗粒(PP)的模拟团聚体的分形维数D f 和预指数因子k n 来表征。用于弹道或扩散受限的粒子群集和群集群集碰撞机制。在此,研究了由16-1024 PP组成的附聚物,其粒度分布受到严格控制(几何标准偏差,<ƒ< sub> g = 1-3)。这些模拟与团聚体的经典结构(D f 和k n )非常吻合,团聚体由四种不同的碰撞机理制成的单分散PP以及bi的团聚体-三分散和正态分布的PP。附聚物的PP尺寸分布变宽,其D f 单调减小,对于足够宽的PP分布(σ g f 不管碰撞机理如何,都达到约1.5,k n 约为1。此外,随着PP多分散性的增加,相应的投影面积指数D α和预指数因子k a 从单分散团聚物的标准值单调降低PP。因此,D f 以及D α和k a 可以指示质量迁移率和光散射测量中的PP多分散性(如果占主导)团聚机理是已知的,例如气溶胶中的扩散受限和/或弹道团簇凝结。

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  • 来源
    《Aerosol Science and Technology》 |2012年第3期|p.347-353|共7页
  • 作者单位

    Particle Technology Laboratory, Institute of Process Engineering, Department of Mechanical and Process Engineering, ETH Zürich, Zürich, Switzerland;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
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  • 入库时间 2022-08-18 00:57:40

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