The simulation of turbulent particle-laden channel flow by the Lattice Boltzmann method
Date of Original Version
We perform direct numerical simulation of three-dimensional turbulent flows in a rectangular channel, with a lattice Boltzmann method, efficiently implemented on heavily parallel general purpose graphical processor units. After validating the method for a single fluid, for standard boundary layer problems, we study changes in mean and turbulent properties of particle-laden flows, as a function of particle size and concentration. The problem of physical interest for this application is the effect of water droplets on the turbulent properties of a high-speed air flow, near a solid surface. To do so, we use a Lagrangian tracking approach for a large number of rigid spherical point particles, whose motion is forced by drag forces caused by the fluid flow; particle effects on the latter are in turn represented by distributed volume forces in the lattice Boltzmann method. Results suggest that, while mean flow properties are only slightly affected, unless a very large concentration of particles is used, the turbulent vortices present near the boundary are significantly damped and broken down by the turbulent motion of the heavy particles, and both turbulent Reynolds stresses and the production of turbulent kinetic energy are decreased because of the particle effects. We also find that the streamwise component of turbulent velocity fluctuations is increased, while the spanwise and wall-normal components are decreased, as compared with the single fluid channel case. Additionally, the streamwise velocity of the carrier (air) phase is slightly reduced in the logarithmic boundary layer near the solid walls.
International Journal for Numerical Methods in Fluids
Banari, Amir, Yackar Mauzole, Tetsu Hara, Stéphan T. Grilli, and Christian F. Janßen. "The simulation of turbulent particle-laden channel flow by the Lattice Boltzmann method." International Journal for Numerical Methods in Fluids 79, 10 (2015): 491-513. doi:10.1002/fld.4058.