Radiation-affected laminar flame propagation

Radiation-Affected Laminar Flame Propagation

where ~ = (Kp/rR ) '~ is the weighted nongreyness, K p and r R are the Planck mean and the Rosseland mean of the absorption coefficient, r = rM6 K is optical thickness, r M = (rprR)'/~ the mean absorption, 8 K the conduction flame thickness, P = 4o TM3/(~5 K) the Planck number, T M the adiabatic flame temperature, ~ the thermal conductivity, and w the albedo, the ratio of scattering to extinction.

Radiation-Affected Laminar Flame Quenching

where p is the density, cp the specific heat at constant pressure, Su the laminar flame speed, Tb the flame temperature, subscript u the unburned gas and superscript 0 the adiabatic gas, ), the thermal conductivity, 7/= (rp/rR)"2 the weighted nongrayness, rp and rR being the Planck mean and the Rosseland mean of the absorption coefficient, ¢. the wall emissitivity, r = rMI the optical thickness...

numerical study on propagation of flame in laminar pre-mixed combustion

premixed combustion is widely used for reducing pollutant emission from combustion chambers. however, these systems may be sensitive to complex phenomena such as flashback. in the present study flame, flashback and structure of premixed laminar flames are investigated theoretically. the mathematical model includes the axi-symmetric continuity, navier stocks, energy, and species equations. combu...

Part II Laminar Flame Dynamics Studies

Single Channel Laminar Flat Flame Simulations

In chapter 5, full 2-D reacting flow simulation of the flat flame burner was reported. A second order fit was found to be appropriate to describe the flame dynamics predicted by the CFD model. However, the phase relationship between the unsteady heat release rate (q′) and the incoming fluid stream velocity fluctuation (u′) was not correctly predicted. Also, the low frequency resonance phenomeno...