Abstract

Using the method of multi-particle collision dynamics (MPCD), we investigate inertial focussing in microfluidic channels that gives rise to the Segré-Silberberg effect. At intermediate Reynolds numbers, we model the motion of a spherical colloid in a circular microchannel under pressure-driven flow. We determine the radial distribution function and show how its width and the location of its maximum are strongly influenced by the colloid size and the Reynolds number of the Poiseuille flow. We demonstrate that MPCD is well suited for calculating mean values for the lift force acting on the colloid in the cross-sectional plane and for its mean axial velocity. We introduce a Langevin equation for the cross-sectional motion whose steady state is the Boltzmann distribution that contains the integrated lift force as potential energy. It perfectly coincides with the simulated radial distribution function.

Highlights

  • In 1962 Segre and Silberberg investigated the behavior of dilute particle suspensions in tube flows at intermediate Reynolds numbers ranging from 7 to 1400 [1,2]

  • We demonstrate that multi-particle collision dynamics (MPCD) is well suited for calculating mean values for the lift force acting on the colloid in the crosssectional plane and for its mean axial velocity

  • In this article we addressed inertial microfluidics using the method of MPCD

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Summary

Introduction

In 1962 Segre and Silberberg investigated the behavior of dilute particle suspensions in tube flows at intermediate Reynolds numbers ranging from 7 to 1400 [1,2]. They observed that the distribution of particles in the crosssection of the tube changed with the distance from the inlet. Even though the injected particles were uniformly distributed, the particles while traveling along the channel moved across streamlines and formed a thin annulus about the centerline of the tube. While the formation of the annulus has been observed previously, Segre and Silberberg were the first to attribute it to fluid inertia. An annulus as observed by Segre and Silberberg cannot form

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