LaboratoryScale Flames
The research approach taken by CCSE has explicitly targeted both the temporal and spatial multiscale aspects of combustion modeling. First, a low Mach number formulation is used instead of the traditional compressible equations, thereby eliminating the acoustic time step restriction while fully maintaining the compressibility effects due to heat release. Second, adaptive mesh refinement (AMR) is used to focus computational resources in regions of interest without wasting resources in regions requiring less resolution. Third, robust integration methods are employed to allow reasonable solution behavior with a minimum of computational resolution. The combination of AMR and a robust low Mach number implementation for reacting flows has reduced the computational requirements of simulating laboratoryscale lowspeed methane combustion by a factor of 10,000 relative to traditional approaches (compressible equations solved on a uniform grid). With these advanced methods, we can simulate timedependent, laboratoryscale, turbulent premixed combustion experiments in three dimensions, while including detailed chemical mechanisms to describe the combustion process and the differential diffusion of the various chemical species.
LaboratoryScale Turbulent Premixed FlamesWithout invoking phenomenological or heuristic models for subgridscale behavior, CCSE's low Mach number model incorporates the detailed chemistry and transport of up to 20 species in this premixed methane flame. The modelled domain includes the entire relevant flow field (tens of centimeters from the nozzle outflow). Additionally, since little is known about the details of the highspeed cold flow within the nozzle itself, we simulate that flow as well using a geometrycapable adaptive model for compressible gas. Results from the auxiliary compressible calculation are coupled into the low Mach simulation through numerical boundary conditions at the inlet plane.
BurkeSchuman Flames (nonpremixed, laminar diffusion flames)We have applied our adaptive low Mach number combustion code to the study of axisymmetric laminar nonpremixed diffusion flames. We have looked at steady and timedependent scenarios for purposes ranging from software validation excercises to detailed pollutant formation analysis. Working in two dimensions, we were able to include a diverse set of combustion chemistry descriptions corresponding to the level of detail necessary for each study. The validation excercises, for example required a reasonable model for ignition chemistry, and were therefore based on a 26species mechanism. Studies geared at understanding gravitational effects on the thermal field from a buouyant flame required only a twostep scheme. And detailed nitrogen pollutant analysis was based on mechanisms that included up to 65 species and 486 reactions. It should be noted that the steady calculations we've performed are not exactly done while operating at our full 'algorithmic strength', in terms of efficiently getting to a solution. Our low Mach simulation algorithm is based on a timedependent model of the flame and fluid physics, so we need to integrate from a simulated startup condition, all the way through to a steady flame. That being said, the refined steady solutions with the largest of mechanisms provided a great deal of spatial information about these BurkeSchumann type flames, including the precise creation and transport mechanisms of nitrogenbased flame intermediates.
Freely Propagating Premixed Hydrogen Flames
Freely Propagating HydrogenMethane Flames
TurbulenceFlame Interactions in Lean Premixed Hydrogen Flames
