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While flame thickness decreases from (0.15 0.07 mm) for stoichiometric mixture at atmospheric pressure.
With the addition of H2/O2, the laminar flame thickness decreases and the growth rate increases.
Increases of the flame thickness up to 10% were observed.
Equivalence ratio has a more dominating effect on adiabatic temperature, density ratio and flame thickness than hydrogen does.
Then the formulation is extended to account for the finite flame thickness, and it is demonstrated how unstable regimes are modified by the flame thickness.
Flame thickness is experimentally shown to vary linearly with K−12.
The results indicate that H2O emission intensity is linearly dependent on flame thickness.
The time-averaged flame thickness was three times as large as the laminar flame.
Flame thickness at the center was measured directly using the luminosity of a SiC filament.
The flame thickness increases with increasing particle size and decreasing pressure.
PLIF images indicate that the flame thickness is on the order of the wake transverse size.
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