Turbulent flame propagation and combustion in spark ignition engines

GP Beretta, M Rashidi, JC Keck - Combustion and flame, 1983 - Elsevier
GP Beretta, M Rashidi, JC Keck
Combustion and flame, 1983Elsevier
Pressure measurements synchronized with high-speed motion picture records of flame
propagation have been made in a transparent piston engine. The data show that the initial
expansion speed of the flame front is close to that of a laminar flame. As the flame expands,
its speed rapidly accelerates to a quasi-steady value comparable with that of the turbulent
velocity fluctuations in the unburned gas. During the quasi-steady propagation phase, a
significant fraction of the gas behind the visible front is unburned. Final burnout of the charge …
Abstract
Pressure measurements synchronized with high-speed motion picture records of flame propagation have been made in a transparent piston engine. The data show that the initial expansion speed of the flame front is close to that of a laminar flame. As the flame expands, its speed rapidly accelerates to a quasi-steady value comparable with that of the turbulent velocity fluctuations in the unburned gas. During the quasi-steady propagation phase, a significant fraction of the gas behind the visible front is unburned. Final burnout of the charge may be approximated by an exponential decay in time.
The data have been analyzed in a model independent way to obtain a set of empirical equations for calculating mass burning rates in spark ignition engines. The burning equations contain three parameters: the laminar burning speed sl, a characteristic speed uT, and a characteristic length lT. The laminar burning speed is known from laboratory measurements. Tentative correlations relating uT and lT to engine geometry and operating variables have been derived from the engine data.
Elsevier
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