EXPERIMENTAL-STUDY AND MODELING OF DODECANE IGNITION IN A DIESEL-ENGINE

Citation
K. Sahetchian et al., EXPERIMENTAL-STUDY AND MODELING OF DODECANE IGNITION IN A DIESEL-ENGINE, Combustion and flame, 103(3), 1995, pp. 207-220
Citations number
35
Categorie Soggetti
Engineering,"Energy & Fuels",Thermodynamics
Journal title
ISSN journal
00102180
Volume
103
Issue
3
Year of publication
1995
Pages
207 - 220
Database
ISI
SICI code
0010-2180(1995)103:3<207:EAMODI>2.0.ZU;2-8
Abstract
Two experiments have been performed under conditions as close as possi ble to those existing in a diesel engine. The first is oxidation of n- dodecane in a motored diesel engine running under conditions close to ignition but avoiding it. The progress of chemical reactions is follow ed by measurements of the global temperature increase Delta T of the e xhaust gases, and by continuous sampling of the combustion chamber gas es, to measure the concentrations of hydroperoxides and molecular hydr ogen; about 4.2% of the energy introduced as hydrocarbon is consumed, thus showing significant transformations during the ignition delay of n-dodecane. The location of the maximum concentration of hydroperoxide s coincides with the fuel jet's edge. Tarlike compounds are present in the unburnt dodecane at the engine exhaust. The second experiment is the study of ignition delay of an n-dodecane spray in an oxidation cha mber filled with air, between 715 and 760 K and 15 and 25 bar. A reduc ed mechanism of 32 reactions, with three types of branching due to the species (RO(2), RO(2)H), (HO2, H2O2), and H, enable one to predict th e ignition delay. Computer simulations are made with the KIVA II code. They show good agreement between the experimental and the calculated ignition delays. They also indicate that, during the ignition delay, r eactions occur first at the boundary of the fuel spray. A temperature increase of about 100 K takes place at the hottest points, which corre spond to concentration maxima of the three branching species. Time-dep endent evolutions of average concentrations show that RO(2)H reaches a maximum first, then H2O2, and lastly the H atom.