TY - JOUR
T1 - DNS study of dependence of bulk consumption velocity in a constant-density reacting flow on turbulence and mixture characteristics
AU - Yu, Rixin
AU - Lipatnikov, Andrei N.
PY - 2017/6/1
Y1 - 2017/6/1
N2 - 3D Direct Numerical Simulation (DNS) study of propagation of a single-reaction wave in forced, statistically stationary, homogeneous, isotropic, and constant-density turbulence was performed in order to evaluate both developing Ut T and fully developed Us T bulk turbulent consumption velocities by independently varying a ratio of 0.5 ≤ u'=SL ≤ 90 of the r.m.s. turbulent velocity to the laminar wave speed and a ratio of 0.39 ≤ L11=δF ≤ 12.5 of the longitudinal integral length scale of the turbulence to the laminar wave thickness. Accordingly, the Damköhler Da = (L11SL)=(u'δF) and Karlovitz Ka = δF=(SLτη) numbers were varied from 0.01 to 24.7 and from 0.36 to 587, respectively. Here, τ is the Kolmogorov time scale. The obtained DNS data show that, at sufficiently low Da, the fully developed ratio of Us T/u' is mainly controlled by Da and scales as p Da. However, such a scaling should not be extrapolated to high Da. The higher Da (or the lower Ka), the less pronounced dependence of Us T/u' on a ratio of L11/δF. Moreover, scaling laws UT α u'αS1-α L(L11=δF)β are substantially different for developing Ut T and fully developed Us T , i.e., the scaling exponents α and, especially, β depend on the wave-development time. Furthermore, α and, especially, depend on a method used to evaluate the developing Ut T . Such effects can contribute to significant scatter of expressions for UT or ST as a function of (u', SL, L11, δF), obtained by parameterizing various experimental databases.
AB - 3D Direct Numerical Simulation (DNS) study of propagation of a single-reaction wave in forced, statistically stationary, homogeneous, isotropic, and constant-density turbulence was performed in order to evaluate both developing Ut T and fully developed Us T bulk turbulent consumption velocities by independently varying a ratio of 0.5 ≤ u'=SL ≤ 90 of the r.m.s. turbulent velocity to the laminar wave speed and a ratio of 0.39 ≤ L11=δF ≤ 12.5 of the longitudinal integral length scale of the turbulence to the laminar wave thickness. Accordingly, the Damköhler Da = (L11SL)=(u'δF) and Karlovitz Ka = δF=(SLτη) numbers were varied from 0.01 to 24.7 and from 0.36 to 587, respectively. Here, τ is the Kolmogorov time scale. The obtained DNS data show that, at sufficiently low Da, the fully developed ratio of Us T/u' is mainly controlled by Da and scales as p Da. However, such a scaling should not be extrapolated to high Da. The higher Da (or the lower Ka), the less pronounced dependence of Us T/u' on a ratio of L11/δF. Moreover, scaling laws UT α u'αS1-α L(L11=δF)β are substantially different for developing Ut T and fully developed Us T , i.e., the scaling exponents α and, especially, β depend on the wave-development time. Furthermore, α and, especially, depend on a method used to evaluate the developing Ut T . Such effects can contribute to significant scatter of expressions for UT or ST as a function of (u', SL, L11, δF), obtained by parameterizing various experimental databases.
U2 - 10.1063/1.4990836
DO - 10.1063/1.4990836
M3 - Article
AN - SCOPUS:85021856287
SN - 1070-6631
VL - 29
JO - Physics of Fluids
JF - Physics of Fluids
IS - 6
M1 - 065116
ER -