By Lin B.-L., Johnson W.B. (eds.)
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Extra resources for Banach Spaces
The initial displacement of the flame is important in the subsequent consumption of the charge and the interaction with in-cylinder turbulence. High-speed Particle Image Velocimetry (HSPIV) has shown that due to the arrangement of the intake ports and pent roof combustion chamber in this type of engine, there is a global flow motion towards the exhaust side of the cylinder near TDC (19). Evidence of this flow motion was visible in all test points apart from Point 1, with the global convection of the flame towards the exhaust side of the cylinder during the 42 expansion stroke.
2. 3% improvement in the fuel consumption over the EIVC and throttled SI operations. 2. All three modes are characterised with very low and nearly constant cycle-to-cycle variability as shown by the COVimep results in Figure 3b. Figure 3c shows that the CAI combustion takes place earlier than the other two modes and it is slightly retarded with the leaner mixture. Though, the CAI operation starts later than the other two modes (Figure 3d) but it is much faster than the EIVC and throttled SI combustion (Figure 3e), due to the simultaneous burning of in-cylinder mixture during the CAI combustion process.
The PN concentration is displayed on the y-axis as dN/dlnD(#/cm3). Combustion Analysis The CAI and EIVC combustion modes were operated with wide open throttle (WOT) and throttled SI at part opened throttle. 3 % reduction in ISFC compared to the throttled SI with the near stoichiometric mixture. 2. 3% improvement in the fuel consumption over the EIVC and throttled SI operations. 2. All three modes are characterised with very low and nearly constant cycle-to-cycle variability as shown by the COVimep results in Figure 3b.