Jm. Donbar et al., Strain rates measured along the wrinkled flame contour within turbulent non-premixed jet flames, COMB FLAME, 125(4), 2001, pp. 1239-1257
The thin, wrinkled CH reaction layers within moderate-(Re = 9,100) and high
- (18,600) Reynolds-number turbulent non-premixed jet flames were identifie
d by using planar laser-induced fluorescence, and the in-plane strain rates
on these reaction layers were measured using simultaneous particle Imaging
Velocimetry (PIV). The PIV diagnostics resolved the Taylor scale; the stra
in-limited diffusion length scale was fully resolved for half the cases stu
died and nearly resolved for the others. In the high-Reynolds-number jet, i
nstantaneous strain rates on the flame surface are highly intermittent, wit
h peak values exceeding 10,000 s(-1). Mean strain rates, conditioned on the
CH-peak contour, are relatively constant (150 s(-1)) in the Re = 9100 flam
e and increase (650-1700 s(-1)) with axial location in the Re = 18,600 flam
e, resulting from the flame wrinkling process. The CH-layer thickness does
not appear to respond in amplitude or in phase with the strain field, indic
ating that quasi-steady conditions do not occur. The strain field apparentl
y oscillates at frequencies as high as 5-10 kHz-which is the inverse of the
crossing time of integral-scale eddies-perhaps because only the low-freque
ncy component of strain effectively acts on the flame. Mean axial velocitie
s, conditioned on the CH-peak contour, were found to remain constant from t
he flame base to tip and to approximately equal the product of the stoichio
metric mixture fraction and the fuel-exit velocity, in agreement with predi
ction. (C) 2001 by The Combustion Institute.