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The Collision Rate of Nonspherical Particles and Aggregates for all Diffusive Knudsen Numbers

机译:所有扩散Knudsen数的非球形粒子和聚集体的碰撞率

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We examine theoretically and numerically collisions of arbitrarily shaped particles in the mass transfer transition regime, where ambiguities remain regarding the collision rate coefficient (collision kernel). Specifically, we show that the dimensionless collision kernel for arbitrarily shaped particles, H, depends solely on a correctly defined diffusive Knudsen number (KnD , in contrast with the traditional Knudsen number), and to determine the diffusive Knudsen number, it is necessary to calculate two combined size parameters for the colliding particles: the Smoluchowski radius, which defines the collision rate in the continuum (KnD →0) regime, and the projected area, which defines the collision rate in the free molecular (KnD →∞) regime. Algorithms are provided to compute these parameters. Using mean first passage time calculations with computationally generated quasifractal (statistically fractal) aggregates, we find that with correct definitions of H and KnD , the H(KnD) relationship found valid for sphere-sphere collisions predicts the collision kernel for aggregates extremely well (to within ±5%). We also show that it is critical to calculate combined size parameters for colliding particles, that is, a collision size/radius cannot necessarily be defined for a nonspherical particle without foreknowledge of the geometry of its collision partner. Specifically for sequentially produced model aggregates, expressions are developed through regression to evaluate all parameters necessary to predict the transition regime collision kernel directly from fractal descriptors.Copyright 2012 American Association for Aerosol ResearchView full textDownload full textRelated var addthis_config = { ui_cobrand: "Taylor & Francis Online", services_compact: "citeulike,netvibes,twitter,technorati,delicious,linkedin,facebook,stumbleupon,digg,google,more", pubid: "ra-4dff56cd6bb1830b" }; Add to shortlist Link Permalink http://dx.doi.org/10.1080/02786826.2012.701353
机译:我们在传质过渡过程中研究了任意形状的粒子的理论和数值碰撞,其中关于碰撞速率系数(碰撞核)的问题仍然不明确。具体而言,我们证明了任意形状的粒子H的无量纲碰撞核仅取决于正确定义的扩散Knudsen数(与传统Knudsen数相比,Kn D ),并确定了扩散克努森数,有必要为碰撞粒子计算两个组合的尺寸参数:Smoluchowski半径和投影面积,Smoluchowski半径定义连续体(Kn D →0)的碰撞率,它定义了自由分子(Kn D →→ˆ)结构中的碰撞率。提供了计算这些参数的算法。使用具有计算生成的准分形(统计分形)集合的平均首次通过时间计算,我们发现,通过正确定义H和Kn D ,可以找到H(Kn D )关系对球体-球体碰撞有效的预测聚集体的碰撞内核非常好(在±5%以内)。我们还表明,计算碰撞粒子的组合尺寸参数非常重要,也就是说,如果不事先了解其碰撞对象的几何形状,则非球面粒子的碰撞尺寸/半径不一定是必需的。专门针对顺序生成的模型集合,通过回归开发表达式,以评估从分形描述符直接预测过渡态碰撞核所需的所有参数。版权所有2012美国气溶胶研究协会查看全文下载全文相关变量var addthis_config = {ui_cobrand:“泰勒和弗朗西斯在线”,services_compact:“ citeulike,netvibes,twitter,technorati,可口,linkedin,facebook,stumbleupon,digg,google,更多”,发布号:“ ra-4dff56cd6bb1830b”};添加到候选列表链接永久链接http://dx.doi.org/10.1080/02786826.2012.701353

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