Turbulence-Induced Relative Velocity of Dust Particles I: Identical Particles

TL;DR

This paper investigates the relative velocities of inertial dust particles in turbulent flows, revealing non-Gaussian velocity distributions and identifying dominant collision mechanisms relevant for protoplanetary disk evolution.

Contribution

It provides a detailed simulation-based analysis of particle relative velocities, validating a predictive model and characterizing the probability distribution functions in turbulent environments.

Findings

The relative velocity PDF is highly non-Gaussian with stretched exponential tails.

The caustic contribution dominates particle collisions at small separations.

Collision kernel peaks at Stokes number around 1, then decreases for larger particles.

Abstract

We study the relative velocity of inertial particles suspended in turbulent flows and discuss implications for dust particle collisions in protoplanetary disks. We simulate a weakly compressible turbulent flow, evolving 14 particle species with friction timescale, tau_p, covering the entire range of scales in the flow. The particle Stokes numbers, St, measuring the ratio of tau_p to the Kolmogorov timescale, are in the range from ~0.1 to ~800. Using simulation results, we show that the model by Pan & Padoan (PP10) gives satisfactory predictions for the rms relative velocity between identical particles. The probability distribution function (PDF) of the relative velocity is found to be highly non-Gaussian. The PDF tails are well described by a 4/3 stretched exponential function for particles with tau_p ~ 1-2 T_L, where T_L is the Lagrangian correlation timescale, consistent with a prediction based on PP10. The PDF approaches Gaussian only for very large particles with tau_p >~ 54 T_L. We split particle pairs at given distances into two types with low and high relative speeds, referred to as continuous and caustic types, respectively, and compute their contributions to the collision kernel. Although amplified by the effect of clustering, the continuous contribution vanishes in the limit of infinitesimal particle distance, where the caustic contribution dominates. The caustic kernel per unit cross section rises rapidly as St increases toward ~1, reaches a maximum at tau_p ~ 2 T_L, and decreases as tau_p^{-1/2} for tau_p >> T_L.