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Fuel Induction Systems for SI Engines. P M V Subbarao Professor Mechanical Engineering Department. The Pace of Net Heat Addition Influence the Area of the Engine Cycle …. Induction of Fuel in SI Engine.
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Fuel Induction Systems for SI Engines P M V Subbarao Professor Mechanical Engineering Department The Pace of Net Heat Addition Influence the Area of the Engine Cycle …..
Induction of Fuel in SI Engine • The task of the engine induction and fuel systems is to prepare from ambient air and fuel in the tank an air-fuel mixture that satisfies the requirement of the engine. • This preparation is to be carried out over entire engine operating regime. • In principle, the optimum air-fuel ratio for an engine is that which give the required power output with the lowest fuel consumption. • It should also ensure smooth and reliable operation. • The fuel Induction systems for SI engine are classified as: • Carburetors. • Throttle body Fuel Injection Systems. • Multi Point Fuel Injection Systems.
pthroat p1 > p2s > pthroat p1 p1 p2s p
Real Flow Through A Venturi pthroat p2a <p2s p1 p1 p2a p
Real Air Flow Through Venturi Where Fuel Flow Through Orifice
Artificial Induction of Fuel • The fuel-injection systems for conventional spark-ignition engines inject the fuel. • There are both mechanical and electronically controlled injection systems. • Better volumetric efficiency • More uniform fuel distribution • More rapid response to changes in loading conditions • More precise control of the equivalence ratio.
Merits of Fuel Injection in the SI Engine • Absence of Venturi – No Restriction in Air Flow/Higher Vol. Eff./Torque/Power • Hot Spots for Preheating cold air eliminated/Denser air enters • Manifold Branch Pipes Not concerned with Mixture Preparation (MPI) • Better Acceleration Response (MPI) • Fuel Atomization Generally Improved. • Use of Greater Valve Overlap • Use of Sensors to Monitor Operating Parameters/Gives Accurate Matching of Air/fuel Requirements: Improves Power, Reduces fuel consumption and Emissions • Precise in Metering Fuel in Ports • Precise Fuel Distribution Between Cylinders (MPI
Merits (Continued) • Fuel Transportation in Manifold not required (MPI) so no Wall Wetting • Fuel Surge During Fast Cornering or Heavy Braking Eliminated • Adaptable and Suitable For Supercharging (SPI and MPI) • Increased power and torque.
Modeling of Fuel injection • The models needs to predict the spray process, • the distribution and evaporation of droplets and • the fuel layer formation and transmission in the port. • The governing equations of motion and droplet evaporation are used to develop a model. • The rate of evaporation of liquid fuel is calculated by first determining the fuel mean drop diameter (SMD) and characteristic evaporation time τeva according below equation: where mlis the liquid fuel mvis the mass of the fuel vapor. eva is time factor
Time Factor • Time factor calculated based on the energy balance between the surrounding air and the liquid droplet and the assumption that the heat transferred is a fraction of the available energy. • The size of droplet and its energy will decide the rate of evaporation.
Droplet Size Distribution • The droplet size distribution in sprays is the crucial parameter needed for the fundamental analysis of the transport of mass, momentum and heat in evaporation. Engineering • Parameter determines the quality of the spray and consequently influences to a significant extent the processes of emissions in combustion. • Detailed experimental data is used to develop distribution functions. • To obtain the detailed quantitative information of the sprays, a two-component Phase Doppler Anemometry (PDA) is used. • This performs the simultaneous measurements of the droplet velocity and size and the volume flux.
Mean diameter distribution of droplets (micron) in 100 mm downstream and 300 Kpa, 25o C
Distribution of droplets velocity (m/s) in 100 mm downstream and 300 Kpa, 25o C
Frequency diagram of droplets mean diameter D is the droplet diameter and N is the normalized number distribution.
Physical Models for Spray Characterization Entropy of a group of droplets: where S is the information entropy, the name used when the information concept is applied to problems in physics and engineering. In this equation K is a constant and Piis the probability of the occurrence of a certain result, in terms of number fraction. Maximum feasible entropy corresponding to physical conditions will decide the droplet distribution.
Physical Constraints • The following physical and mathematical constraints must be obeyed: • The sum of all probabilities must be unity: (ii) the mass flow of sprayed liquid must be equal to the mass of all droplets produced per unit time: where n is the total number of droplets produced per unit time and mL is the liquid mass flux.