Experimental study of the influence of Lewis number, laminar flame thickness, temperature, and pressure on turbulent flame speed using hydrogen and methane fuels

To experimentally explore the influence of Lewis number , laminar flame thickness , pressure , and unburned gas temperature on turbulent flame speed , a set of conditions is designed by adjusting nitrogen mole fraction in lean H/O/N () and stoichiometric CH/O/N () mixtures. The adjustment is performed by simulating complex-chemistry laminar flames to obtain the same laminar flame speeds not only for different fuels, but also for different pressures (1, 2, and 5 atm). The mixtures are characterized by significantly different at K and 400 K, whereas variations in with the temperature are sufficiently weak. Moreover, laminar flame thicknesses are approximately equal for H-based and CH-based mixtures at the same , but are significantly decreased with increasing pressure. For this set of conditions, is measured by applying schlieren imaging techniques to film expansion of centrally ignited, statistically spherical flames in homogeneous isotropic turbulence generated by a dual-chamber, constant-pressure, fan-stirred explosion facility. Analyses of the measured data show the following trends. First, turbulent flame speed is increased by both and , whereas is decreased with increasing . Second, turbulent flame speed measured at different and can be predicted by allowing for and . Thus, the present data do not call for explicitly substituting normalized pressure or temperature into a turbulent flame speed approximation. Third, is increased with decreasing laminar flame thickness. Fourth, speeds of the lean H/O/N flames are higher when compared to the stoichiometric CH/O/N flames, with this difference is increased (reduced) by (, respectively). Fifth, all measured data on can quantitatively be described by substituting and with the counterpart characteristics of highly strained twin laminar flames. The latter finding supports leading point concept of premixed turbulent combustion.