By D. Siano
ISBN-10: 9533071168
ISBN-13: 9789533071169
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Example text
Kroger H. y Ganser J. (1991) “Detection of Knocking of Combustion Using Simultaneously High Speed Schlieren Cinematography and Multi- Optical Fibre Techique". SAE Technical Paper 912312. , Urushihara T. y Naitoh K. (1998) “Simultaneous Attainment of low Fuel Consumption, High Output Power and Low Exhaust Emissions in Direct Injection SI Engines". SAE Technical Paper 980149. Tinaut F. , Sanchez M. L. y Gimenez B. (1993) Visualization and Measurement of Speed and Size in Diesel Sprays, pp. 78-83.
157-174. Atomization and Sprays. , Minamia T. y Yokota K. (1997) “Measurement of Liquid Phase Penetration of Evaporating Spray in a DI Diesel Engine". SAE Technical Paper 971645. Zhao F. , Kadota T. y Takemoto T. (1991) “Temporal and Cyclic Fluctuation of Fuel Vapor Concentration in a Spark Ignition Engine". SAE Technical Paper 912346.
Furthermore, the suggested correlation illustrates important details about how the main parameters affect the fuel injection process. The nozzle diameter has the greatest effect on liquid penetration length. A reduction in nozzle diameter yields a shorter penetration length because it causes an earlier start of the second break-up regime. Increasing the injection pressure provokes premature droplet break-up within the jet, which results mainly due to cavitation at the nozzle exit. If the working fluid density in the combustion chamber increases the penetration length is shorter and the second break-up regime is delayed due to the free-share flow between the working fluid and the fuel jet, which produces higher evaporation rates of droplets from the diesel jet.
Fuel Injection by D. Siano
by Steven
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