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Direct Numerical Simulation of Autoignition in a Jet in a Cross-Flow ...

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1.1.1 Summary <strong>of</strong> <strong>Numerical</strong> <strong>Simulation</strong>sExploratory numerical simulations on experimental computational grids as well asproduction runs were performed dur<strong>in</strong>g the early science period on Mira. The computationalgrid is composed <strong>of</strong> N E = 1, 591, 752 spectral elements with<strong>in</strong> which thesolution is <strong>in</strong>terpolated us<strong>in</strong>g three-dimensional tensorial product <strong>of</strong> p=6-th orderLagrange polynomials.Post process<strong>in</strong>g <strong>of</strong> the solution was performed us<strong>in</strong>g NEK5000 on the twodatasets <strong>in</strong>clud<strong>in</strong>g computations <strong>of</strong> key species generation rates, mixture fraction,scalar dissipation rate, Takeno flame <strong>in</strong>dex and vorticity components. Analysis<strong>of</strong> the two large data sets was also ma<strong>in</strong>ly facilitated through visualizations withVisIt on the ALCF’s GPU system (Eureka). Two crossflow stream temperatures(T cf =930 and 950 K) were simulated at a Reynolds number, based on the frictionvelocity and the channel half-width, <strong>of</strong> Re τ = 180. Typical <strong>in</strong>stantaneous snapshots<strong>of</strong> the fully ignited case are shown <strong>in</strong> fig. 1.1.The simulations performed up till now employed close to 345 million gridpo<strong>in</strong>ts correspond<strong>in</strong>g to 4.8 billion degrees <strong>of</strong> freedom (14 unknowns per gridpo<strong>in</strong>t). We are currently develop<strong>in</strong>g the computational mesh for a planned highReynolds number simulation (Re τ = 590). It is estimated that the total number <strong>of</strong>elements will be close to 3 millions and the polynomial order will be at least 8.3

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