Structure and propagation of two-dimensional, partially premixed, laminar flames in diesel engine conditions

Abstract  We investigate the influence of inflow velocity ( V in ) and scalar dissipation rate ( χ ) on the flame structure and stabilisation mechanism of steady, laminar partially premixed n -dodecane edge flames stabilised on a convective mixing layer. Numerical simulations were performed for three different χ profiles and several V in ( V in = 0.2 to 2.5m/s). The ambient thermochemical conditions were the same as the Engine Combustion Network’s (ECN) Spray A flame, which in turn represents conditions in a typical heavy duty diesel engine. The results of a combustion mode analysis of the simulations indicate that the flame structure and stabilisation mechanism depend on V in and χ . For low V in the flame is attached. Increasing V in causes the high-temperature chemistry (HTC) flame to lift-off, while the low-temperature chemistry (LTC) flame is still attached. A unique speed S R associated with this transition is defined as the velocity at which the lifted height has the maximum sensitivity to changes in V in . This transition velocity is negatively correlated with χ . Near V i n = S R a tetrabrachial flame structure is observed consisting of a triple flame, stabilised by flame propagation into the products of an upstream LTC branch. Further increasing the inlet velocity changes the flame structure to a pentabrachial one, where an additional HTC ignition branch is observed upstream of the triple flame and ignition begins to contribute to the flame stabilisation. At large V in , the LTC is eventually lifted, and the speed at which this transition occurs is insensitive to χ . Further increasing V in increases the contribution of ignition to flame stabilisation until the flame is completely ignition stabilised. Flow divergence caused by the LTC branch reduces the χ at the HTC branches making the HTC more resilient to χ . The results are discussed in the context of identification of possible stabilisation modes in turbulent flames.