GRADIENT AND COUNTER-GRADIENT SCALAR TRANSPORT IN TURBULENT PREMIXED FLAMES

In premixed turbulent combustion, the modelling of the turbulent flux of the mean reaction progress variable, (c) over tilde, <(rho u(i) '' c '')over bar>, remains somewhat controversial. Classical gradient tra nsport assumptions based on the eddy viscosity concept are often used while both experimental data and theoretical analysis have pointed out the existence of counter-gradient turbulent diffusion. Direct numeric al simulation (DNS) is used in this paper to provide basic information on the turbulent flux of (c) over tilde and study the occurrence of c ounter-gradient transport. The numerical configuration corresponds to two- or three-dimensional premixed flames in isotropic turbulent flow. The simulations correspond to various flame and flow conditions that are representative of flamelet combustion. They reveal that different flames will feature different turbulent transport properties and that these differences can be related to basic dynamical differences in the flame-flow interactions: counter-gradient diffusion occurs when the f low field near the flame is dominated by thermal dilatation due to che mical reaction, whereas gradient diffusion occurs when the flow field near the flame is dominated by the turbulent motions. The DNS-based an alysis leads to a simple expression to describe the turbulent flux of (c) over tilde, which in turn leads to a simple criterion to delineate between the gradient and counter-gradient turbulent diffusion regimes . This criterion suggests that the occurrence of one regime or the oth er is determined primarily by the ratio of turbulence intensity divide d by the laminar flame speed, u'/s(L), and by the flame heat release f actor, tau = (T-b - T-u)/T-u, where T-u and T-b are respectively the t emperature within unburnt and burnt gas. Consistent with the Bray-Moss -Libby theory, counter-gradient (gradient) diffusion is promoted by lo w (high) values of u'/s(L) and high (low) values of tau. DNS also show s that these results are not restricted to the turbulent transport of (c) over tilde. Similar results are found for the turbulent transport of flame surface density, C. The turbulent fluxes of (c) over tilde an d Sigma are strongly correlated in the simulated flames and counter-gr adient (gradient) diffusion of (c) over tilde always coincides with co unter-gradient (gradient) diffusion of C.