Modeling of Emissions in a Laboratory Swirl Combustor

Author(s):  
Viswanath R. Katta ◽  
William M. Roquemore

A swirl-stabilized combustor utilizes recirculation zones for stabilizing the flame. The performance of such combustors could depend on the fuel used as the cracked fuel products may enter the recirculation-zones and alter their characteristics. A numerical study is conducted for understanding the effects of fuel variation on the combustion and unburned-hydrocarbon-emission characteristics of a laboratory swirl combustor. A time-dependent, detailed-chemistry CFD model UNICORN is used. Six binary fuel mixtures formulated with n-dodecane and n-heptane, m-xylene, iso-octane or hexadecane are considered. A semi-detailed chemical-kinetics model (CRECK-0810) involving 206 species and 5652 reactions for the combustion of these fuels is incorporated into UNICORN code. Calculations are performed for a fuel-lean condition, which represents cruise operation of an aircraft. Combustor flows simulated with different fuel mixtures yielded nearly the same flowfields and flame structures. Production of the intermediate cracked fuel species that are key for the final flame structure and emissions seems to be independent of the fuel used. This finding could greatly simplify the detailed chemical kinetics used for obtaining cracked products. As the cracked fuel species are completely consumed with in the flame zone, no emissions are observed at the combustor exit for the considered fuel-lean condition.

Author(s):  
Viswanath R. Katta ◽  
William M. Roquemore

Swirl-stabilized combustor utilizes recirculation zones for stabilizing the flame. A numerical study is conducted for understanding the effect of recirculation zones on the combustion of practical fuels in this burner. A time-dependent, detailed-chemistry CFD model UNICORN is used. JP-8 fuel is modeled using two independently proposed surrogate mixtures. A semi-detailed chemical-kinetics model involving 161 species and 1538 reactions is incorporated into UNICORN code for describing the combustion of these surrogate mixtures. Calculations are performed for fuel-lean, stoichiometric, and fuel-rich conditions. Flames simulated with different surrogate mixtures in all three equivalence-ratio cases yielded nearly the same structures even though the two surrogate mixtures are very different in chemical composition. For understanding the role of individual parent species in the surrogate mixtures, calculations for the swirl combustor are repeated after replacing the surrogate fuel with one of its parent species. Detailed comparisons of flames generated with different parent species revealed significant variations in flame structures. However, the flames generated by the surrogate mixtures are nearly similar—suggesting that these mixtures are formulated for representing the same JP-8 fuel.


Author(s):  
A. I. Lopato ◽  
◽  
A. G. Eremenko ◽  

Recently, we developed a numerical approach for the simulation of detonation waves on fully unstructured grids and applied it to the numerical study of the mechanisms of detonation initiation in multifocusing systems. Current work is devoted to further development of our numerical approach, namely, parallelization of the numerical scheme and introduction of more comprehensive detailed chemical kinetics scheme.


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