US EPA

1187508 

Journal Article 

Self-ignition of SI engine model fuels: A shock tube investigation at high pressure 

Fieweger, K; Blumenthal, R; Adomeit, G 

1997 

Yes 

Combustion and Flame
ISSN: 0010-2180 

109 

4 

599-619 

10.1016/S0010-2180(97)00049-7 

WOS:A1997XA78600008 

The self-ignition of several spark-ignition (SI) engine fuels (iso-octane, methanol, methyl tert-butyl ether and three different mixtures of iso-octane and n-heptane), mixed with air, was investigated experimentally under relevant engine conditions by the shock tube technique. Typical modes of the self-ignition process were registered cinematographically. For temperatures relevant to piston engine combustion, the self-ignition process always starts as an inhomogeneous, deflagrative mild ignition. This instant is defined by the ignition delay time, tau(defl). The deflagration process in most cases is followed by a secondary explosion (DDT). This transition defines a second ignition delay time, tau(DDT) which is a suitable approximation for the chemical ignition delay time, if the change of the thermodynamic conditions of the unburned test gas due to deflagration is taken into account. For iso-octane at p = 40 bar, a NTC (negative temperature coefficient), behaviour connected with a two step (cool flame) self-ignition at low temperatures was observed. This process was very pronounced for rich and less pronounced for stoichiometric mixtures. The results of the tau(DDT) delays of the stoichiometric mixtures were shortened by the primary deflagration process in the temperature range between 800 and 1000 K. Various mixtures of iso-octane and n-heptane were investigated. The results show a strong influence of the n-heptane fraction in the mixture, both on the ignition delay time and on the mode of self-ignition. The self-ignition of methanol and MTBE(methyl tert-butyl ether) is characterized by a very pronounced initial deflagration. For temperatures below 900 K (methanol: 800 K), no secondary explosion occurs. Taking into account the pressure increase due to deflagration, the measured delays tau(DDT) of the secondary explosion are shortened by up to one order of magnitude. (C) 1997 by The Combustion Institute.