# Statistics of particle accumulation in spatially developing turbulent   boundary layers

**Authors:** Gaetano Sardina, Francesco Picano, Philip Schlatter, Luca Brandt and, Carlo Massimo Casciola

arXiv: 1703.10433 · 2017-03-31

## TL;DR

This study uses direct numerical simulation to analyze how inertial particles behave in a spatially developing turbulent boundary layer, revealing how local flow parameters and flow structures influence particle distribution and accumulation.

## Contribution

It provides new insights into particle dynamics in developing boundary layers, highlighting the effects of streamwise variation and flow structures on particle accumulation.

## Key findings

- Minimum particle concentration occurs inside the boundary layer.
- Particle behavior depends on local Stokes numbers and flow regions.
- Flow structures influence particle transport and accumulation.

## Abstract

We present the results of a Direct Numerical Simulation of a particle-laden spatially developing turbulent boundary layer up to Re{\theta} = 2500. Two main features differentiate the behavior of inertial particles in a zero- pressure-gradient turbulent boundary layer from the more commonly studied case of a parallel channel flow. The first is the variation along the streamwise direction of the local dimensionless parameters defining the fluid-particle in- teractions. The second is the coexistence of an irrotational free-stream and a near-wall rotational turbulent flow. As concerns the first issue, an inner and an outer Stokes number can be defined using inner and outer flow units. The inner Stokes number governs the near-wall behavior similarly to the case of channel flow. To understand the effect of a laminar-turbulent interface, we ex- amine the behavior of particles initially released in the free stream and show that they present a distinct behavior with respect to those directly injected inside the boundary layer. A region of minimum concentration occurs inside the turbulent boundary layer at about one displacement thickness from the wall. Its formation is due to the competition between two transport mecha- nisms: a relatively slow turbulent diffusion towards the buffer layer and a fast turbophoretic drift towards the wall.

## Full text

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## Figures

18 figures with captions in the complete paper: https://tomesphere.com/paper/1703.10433/full.md

## References

21 references — full list in the complete paper: https://tomesphere.com/paper/1703.10433/full.md

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Source: https://tomesphere.com/paper/1703.10433