4.6 Article

Modeling particle-particle binary coagulation rate constants for spherical aerosol particles at high volume fractions using Langevin Dynamics simulations

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JOURNAL OF AEROSOL SCIENCE
卷 164, 期 -, 页码 -

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ELSEVIER SCI LTD
DOI: 10.1016/j.jaerosci.2022.106001

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  1. UMRF Ventures Professorship

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The effect of volume fraction and particle-particle hydrodynamic interactions on the coagulation rate of particles is investigated in this study. Langevin Dynamics based trajectory simulations are used to model particle coagulation, and the Kirkwood-Risemann approach is employed to calculate particle-particle hydrodynamic interactions. The results show that the coagulation rate constant depends on the diffusive Knudsen number, momentum Knudsen number, and particle volume fraction.
Effect of volume-fraction and particle-particle hydrodynamic interactions on the coagulation rate of particles are investigated. Particle coagulation is modeled using Langevin Dynamics (LD) based trajectory simulations of N mono-sized spherical particles in a periodic domain. The extended Kirkwood-Risemann approach (J. Fluid Mechanics 855, 535 (2018)) is invoked to compute particle-particle hydrodynamic interactions whose effect is parameterized as a function of the momentum Knudsen number (Kn). The results are summarized as a model for coagulation rate constant (beta ij) that depends on the diffusive Knudsen number (KnD) used in prior work to parameterize coagulation in the dilute regime (Aerosol Sci. Tech. 45, 1499 (2011)), Kn and particle volume-fraction eta v. In the absence of hydrodynamic interactions, it is observed that the coagulation rate constant in the continuum limit for mass transfer (KnD -> 0) is significantly enhanced by a factor of-80 at eta v <- 0.3 due to particle crowding. While considering hydrodynamic interactions for eta v & GE; 0.05, we use a screening distance around each particle that scales inversely with eta v beyond which the contribution of farther neighbors is neglected owing to the rapid decay of hydrodynamic interactions with distance. We also present new LD calculations of beta ij and elucidate the dependence of the same on Kn1 and the particle radii ratio theta r for the coagulation of two particles in the dilute limit eta v & RARR; 0. It is observed that the reduction of beta ij becomes significant as Kn1 & RARR; 0: at the lowest momentum Knudsen number considered (Kn1 = 0.1): beta ij is reduced by a factor of-10 for equally sized particles (theta r = 0.5). At high KnD,Kn1, the particle size disparity is not significant, and it is seen that beta ij matches hard sphere predictions, indicating the insignificant contributions by hydrodynamic interactions. A series of animations of 2 particle simulations are presented as part of the Supplemental Information to illustrate the role of hydrodynamic interactions in particle coagulation. Computational results are summarized as regressions for convenient incorporation into particle/droplet growth sectional models.

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