Unstructured LES of Reacting Multiphase Flows in Realistic Gas Turbine Combustors

As part of the Accelerated Strategic Computing Initiative (ASCI) program, an accurate and robust simulation tool is being developed to perform high-fidelity LES studies of multiphase, multiscale turbulent reacting flows in aircraft gas turbine combustor configurations using hybrid unstructured grids. In the combustor, pressurized gas from the upstream compressor is reacted with atomized liquid fuel to produce the combustion products that drive the downstream turbine. The Large Eddy Simulation (LES) approach is used to simulate the combustor because of its demonstrated superiority over RANS in predicting turbulent mixing, which is central to combustion. This paper summarizes the accomplishments of the combustor group over the past year, concentrating mainly on the two major milestones achieved this year: 1) Large scale simulation: A major rewrite and redesign of the flagship unstructured LES code has allowed the group to perform large eddy simulations of the complete combustor geometry (all 18 injectors) with over 100 million control volumes; 2) Multi-physics simulation in complex geometry: The first multi-physics simulations including fuel spray breakup, coalescence, evaporation, and combustion are now being performed in a single periodic sector (1/18th) of an actual Pratt & Whitney combustor geometry.

[1]  C. Edwards,et al.  Quasi-steady deformation and drag of uncontaminated liquid drops , 2002 .

[2]  Marcus Herrmann,et al.  Modeling Primary Breakup: A Three-Dimensional Eulerian Level Set/Vortex Sheet Method for Two-Phase Interface Dynamics , 2003 .

[3]  J. Oefelein Simulation and analysis of turbulent multiphase combustion processes at high pressures , 1997 .

[4]  Parviz Moin,et al.  A semi-implicit method for resolution of acoustic waves in low Mach number flows , 2002 .

[5]  J. Dukowicz A particle-fluid numerical model for liquid sprays , 1980 .

[6]  K. Mahesh,et al.  A Eulerlan-Lagrangian Model to Simulate Two-Phase/Particulate Flows , 2003 .

[7]  Dimitri J. Mavriplis,et al.  AIAA 99 – 0537 LARGE-SCALE PARALLEL UNSTRUCTURED MESH COMPUTATIONS FOR 3 D HIGH-LIFT ANALYSIS , 1999 .

[8]  C. Pierce,et al.  Progress-variable approach for large-eddy simulation of turbulent combustion , 2001 .

[9]  P. Moin,et al.  Large-eddy simulation of swirling particle-laden flows in a coaxial-jet combustor , 2003 .

[10]  Gerard M. Faeth,et al.  CURRENT STATUS OF DROPLET AND LIQUID COMBUSTION , 1977 .

[11]  Robert D. Falgout,et al.  hypre: A Library of High Performance Preconditioners , 2002, International Conference on Computational Science.

[12]  D. Metzger,et al.  Measurements in turbulent swirling flow through an abrupt axisymmetric expansion , 1988 .

[13]  Martin Sommerfeld,et al.  Detailed measurements in a swirling particulate two-phase flow by a phase-Doppler anemometer , 1991 .

[14]  G. Faeth Evaporation and combustion of sprays , 1983 .

[15]  Heinz Pitsch,et al.  Consistent boundary conditions for integrated LES/RANS simulations: LES outflow conditions , 2002 .

[16]  P. Moin,et al.  LES of atomizing spray with stochastic modeling of secondary breakup , 2002 .

[17]  M. Sommerfeld,et al.  Multiphase Flows with Droplets and Particles , 2011 .

[18]  P. Moin,et al.  A dynamic subgrid‐scale model for compressible turbulence and scalar transport , 1991 .

[19]  Martin Sommerfeld,et al.  Experimental studies of spray evaporation in turbulent flow , 1998 .

[20]  Brian T. Helenbrook,et al.  A two-fluid spectral-element method , 2001 .