GAS-DYNAMIC FEATURES OF SELF-IGNITION OF NON DILUTED FUEL AIR MIXTURES AT HIGH-PRESSURE/

Citation
R. Blumenthal et al., GAS-DYNAMIC FEATURES OF SELF-IGNITION OF NON DILUTED FUEL AIR MIXTURES AT HIGH-PRESSURE/, Combustion science and technology, 114, 1996, pp. 137-166
Citations number
19
Categorie Soggetti
Energy & Fuels",Engineering,Thermodynamics
ISSN journal
00102202
Volume
114
Year of publication
1996
Pages
137 - 166
Database
ISI
SICI code
0010-2202(1996)114:<137:GFOSON>2.0.ZU;2-Z
Abstract
The self ignition of several non diluted fuel/air mixtures at high pre ssure is studied. Hydrogen, iso-octane and n-heptane have been used as fuels. Experiments have been performed using the shock tube technique . Various observation methods, such as recording of pressure and of li ght band emission and shadow cinematography have been applied. The typ e of self ignition as well as the ignition delay times can be determin ed using these techniques; The self ignition of all fuels takes place in many different modes. At high temperatures ignition at the end wall is achieved. All three fuels under investigation show mild and strong ignition as described by Oppenheim (1985). Mild ignition - characteri zed by establishing a deflagrative combustion mode at seperate indepen dent reaction centers - also occurs at low temperatures, when the igni tion process is - within some limits-randomly distributed in rime and space (hot spot ignition). Hydrogen shows this hot spot ignition with and without transition to detonation (DDT). In the case of n-heptane t he hot spot ignition always ends up in a transition to detonation. The iso-octane/air mixture exhibits very clearly both ignition modes with and without DDT. The fuels n-heptane and iso-octane both show in the regime of mild ignition flame zones with spherical or planar structure , depending on the temperature. The planar structure, so far, has not been observed for hydrogen. It seems that this behavior can be explain ed by the sensitivity of the chemical system to disturbances in temper ature. This interpretation can be regarded as an extension to the cohe rence theory explaining the strong ignition limit (Meyer and Oppenheim , 1971b).