A Coupling Algorithm for Eulerian- Lagrangian Simulation of Dense Gas- Solid Reacting Flows on Unstructured Mesh Jian Cai Assistant Professor University of Wyoming
Combustion research at UW New combustion program □ Mechanical Engineering Department □ Four junior faculty members □ Coal utilization Research topics □ Laser spectroscopy □ Turbulent combustion experiments and modeling □ Pulverized and dense coal combustion □ Radiation modeling and measurements 2
Coal combustion and gasification What is the limiting factor for accuracy? What is the next limiting factor? 3 TurbulenceRadiation MultiphaseChemistry
E-L models for multiphase flows Advantages in accounting for changes of □ Particle size and distribution Heat transfer Heterogeneous reactions □ History between different particles Composition Temperature Disadvantages □ Computational cost □ Unknown surface properties 4
OpenFOAM Lagrangian existing capabilities □ Pulverized coal combustion □ Collisional non-reacting particles Eulerian □ Solving transport equations □ Needs a new coupling algorithm 5
FVM: unstructured collocated mesh 6
Coupled equations ModelCoupling variables IncompressibleU, p CompressibleU, p, T, ρ Multiphase compressibleU, p, T, ρ, ε 7
Coupling algorithm 8 Energy, species equations + Equation of state Density update Velocity-pressure coupling
Reacting test case 9 Pseudo 2D DPM Char 2.5mm parcels 3s physical time
CFB Zhou et al CES MPPIC Sand 213µm 0.3Mparcel x 1000p/parcel 10
Particle volume fraction 11
Conclusions Eulerian-Lagrangian coupling algorithm □ Unstructured collocated mesh □ Gas-solid dense reacting flows Computational cost is the major limitation □ MPPIC faster than DPM 12