Particle chirality does not matter in the large-scale features of strong turbulence
arXiv:2404.04217 · doi:10.1017/jfm.2024.577
Abstract
We use three-dimensional direct numerical simulations of homogeneous isotropic turbulence in a cubic domain to investigate the dynamics of heavy, chiral, finite-size inertial particles and their effects on the flow. Using an immersed-boundary method and a complex collision model, four-way coupled simulations have been performed, and the effects of particle-to-fluid density ratio, turbulence strength and particle volume fraction have been analysed. We find that freely falling particles on the one hand add energy to the turbulent flow but, on the other hand, they also enhance the flow dissipation: depending on the combination of flow parameters, the former or the latter mechanism prevails, thus yielding enhanced or weakened turbulence. Furthermore, particle chirality entails a preferential angular velocity which induces a net vorticity in the fluid phase. As turbulence strengthens, the energy introduced by the falling particles becomes less relevant and stronger velocity fluctuations alter the solid phase dynamics, making the effect of chirality irrelevant for the large-scale features of the flow. Moreover, comparing the time history of collision events for chiral particles and spheres (at the same volume fraction) suggests that the former tend to entangle, in contrast to the latter which rebound impulsively.
References in corpus (8)
- Sedimentation of finite-size spheres in quiescent and turbulent environments
- Laminar, turbulent and inertial shear-thickening regimes in channel flow of neutrally buoyant particle suspensions
- Forcing homogeneous turbulence in DNS of particulate flow with interface resolution and gravity
- Supergravitational turbulent thermal convection
- Statistical models for the dynamics of heavy particles in turbulence
- Chiral Active Particles are Sensitive Reporter to Environmental Geometry
- The effect of particle anisotropy on the modulation of turbulent flows
- Strong alignment of prolate ellipsoids in Taylor-Couette flow