507765 Modeling of Heat and Momentum Transfer in the Context of Moving Particles By a Double MRT Lattice Boltzmann Scheme

Bogdan Kravets, Mechanical Process Engineering and Solids Processing (MVTA), Technical University Berlin (TU Berlin), Berlin, Germany and Harald Kruggel-Emden, Department of Energy Plant Technology, Ruhr-Universitaet Bochum, Bochum, Germany

Modeling of Heat and Momentum Transfer in the Context of Moving Particles by a Double MRT Lattice Boltzmann Scheme Bogdan Kravets, Harald Kruggel-Emden

Mechanical Process Engineering and Solids Processing (MVTA)

Technical University Berlin (TU Berlin)

Ernst-Reuter-Platz 1, 10587 Berlin, Germany

e-mail: kravets@tu-berlin.de, kruggel-emden@tu-berlin.de, web page: http://www.mvta.tu-berlin.de

ABSTRACT

Dynamic particle/fluid systems - like in fluidized beds, in pneumatic conveying or in rotary kilns passed through by a fluid - occur in many areas of technical processes in chemical industry and in energy technology. Modeling of the named systems gained in significance during the past years [1–5]. The most common applicable approach is the discrete element method (DEM) coupled with computational fluid dynamics (CFD), where the solid phase is described by Newton's laws of motion and the fluid phase by the Navier-Stokes equations. However, coupled DEM/CFD usually does not resolve the fluid phase spatially around individual particles.

Particle resolved flow simulations can rely on Navier-Stokes (NS) based approaches like finite volume method (FVM) or finite difference method (FDM) or more alternative schemes like the Lattice-Boltzmann method (LBM). Unlike other direct numerical simulation (DNS) methods, LBM is not solving Navier-Stokes equations but is based on kinetic theory and the discrete Boltzmann equation. LBM utilizes a Cartesian mesh and hence does not require a complex mesh derivation or a re-meshing when boundaries are moving. To address coupled heat transfer and fluid flow conventional LBM can be extended by thermal LBM (TLBM). The resulting scheme relies on a set of two distribution functions, the so called double distribution function (DDF) approach [6]; one for the fluid density and one for the internal energy.

For the carried out numerical investigations an existing 3D TLBM framework which was utilized for static particle packing simulations [7,8] in the past is extended for moving particles. Both, the fluid field and the temperature field are represented by a multiple-relaxation-time (MRT) [9–11] collision operator. For the hydrodynamic boundary conditions, a scheme introduced by Bouzidi et al. [12] is applied with quadratic interpolation. Thermal boundary conditions are prescribed according to Li et al. [13] with linear interpolation. The used boundary conditions are superior to the standard half way bounce back and are suitable for curved boundaries. Particle interactions are taken care of in the context of the DEM. The numerical TLBM framework is applied to moving particles and is validated against available analytical solutions and results obtained from the scientific literature. It is shown that the derived framework offers a highly accurate and efficient approach for the analysis of moving particles considering heat transfer problems under resolved flow.

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