Scalar filtered mass density functions in nonpremixed turbulent jet flames

• Published in: Combustion and flame 2008-10, Vol.155 (1), p.54-69
• Main Authors: Drozda, Tomasz G., Wang, Guanghua, Sankaran, Vaidyanathan, Mayo, Jackson R., Oefelein, Joseph C., Barlow, Robert S.
• Format: Article
• Language: English
• Subjects: Applied sciences; Combustion of gaseous fuels; Combustion. Flame; DENSITY; DIGITAL FILTERS; Energy; Energy. Thermal use of fuels; Exact sciences and technology; EXPERIMENTAL DATA; Filtered density function; Filtered density functions; FLAMES; Fluid dynamics; Fluid flow; FUNCTIONS; HYDROGEN; INORGANIC, ORGANIC, PHYSICAL AND ANALYTICAL CHEMISTRY; Jet flames; JETS; KERNELS; MASS; METHANE; MIXTURES; NITROGEN; ONE-DIMENSIONAL CALCULATIONS; Raman/Rayleigh/LIF; REYNOLDS NUMBER; SCALARS; SHAPE; Theoretical studies. Data and constants. Metering; TURBULENCE; Turbulent flames; Turbulent flow; Turbulent jet flame; Variance
• ISSN: 0010-2180; 1556-2921
• DOI: 10.1016/j.combustflame.2008.06.012

Filtered mass density functions (FMDFs) of mixture fraction and temperature are studied by analyzing experimental data obtained from one-dimensional Raman/Rayleigh/LIF measurements of nonpremixed CH 4/H 2/N 2 turbulent jet flames at Reynolds numbers of 15,200 and 22,800 (DLR-A and -B). The experimentally determined FMDFs are conditioned on the Favré filtered values of the mixture fraction and its variance. Filter widths are selected as fixed multiples of the experimentally determined dissipation length scale at each measurement location. One-dimensional filtering using a top-hat filter is performed to obtain the filtered variables used for conditioning. The FMDFs are obtained by binning the mass and filter kernel weighted samples. Emphasis is placed on the shapes of the FMDFs in the fuel-rich, fuel-lean, and stoichiometric intervals for the Favré filtered mixture fraction, and low, medium, and high values for the Favré filtered mixture fraction variance. It is found that the FMDFs of mixture fraction are unimodal in samples with low mixture fraction variance and bimodal in samples with high variance. However, the FMDFs of mixture fraction at the smallest filter size studied are unimodal for all values of the variance. The FMDFs of temperature are unimodal in samples with low mixture fraction variance, and either unimodal or bimodal, depending on the mixture fraction mean, in samples with high variance. The influence of the filter size and the jet Reynolds number on the FMDFs is also considered.