2022年《发动机原理》双语教案2.pdf
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1、Chapter 4 Combustion in Spark Ignition Engines Key: Mixture formation way of SI engine, combustion phenomenon of SI engine, design of SI engine combustion chamber. Difficult points: Gasoline engine abnormal combustion phenomenons and influence factors Section 1 Introduction to spark ignition engineI
2、n SI engines the air and fuel are usually mixed together in the intake system prior to entry to the engine cylinder, using a carburetor or fuel-injection system. The electronic fuel injection system has the job of supplying a combustible mixture of air and fuel to the engine. This typical system can
3、 be divided into three parts: fuel delivery system, air induction system, and the electronic control system. 1.Air induction system When the throttle valve is opened, air flows through the air cleaner, through the air flow meter, past the throttle valve, and through a well-tuned intake manifold runn
4、er to the intake valve. 2.fuel delivery system Fuel is delivered from tank to the injector by means of an electric fuel pump. Contaminants are filtered out by a high capacity in line fuel filter. Fuel is maintained at a constant pressure by means of a fuel pressure regulator. Any fuel which is not d
5、elivered to the intake manifold by the injector is returned to the tank through a fuel return pipe. 3.electronic control system The ECU determines precisely how much fuel needs to be delivered by the injector by monitoring the engine sensors. The ECU turns the injectors on for a precise amount of ti
6、me , referred to as injection pulse width or injection duration, to deliver the proper air-fuel ratio to the engine. Section 2 Combustion phenomenon Combustion either occurs normally - with ignition from a spark and the flame front propagating steadily throughout the mixture - or abnormally. 4.2.1 N
7、ormal combustion When the piston approaches the end of the compression stroke, a spark is discharged between the sparking plug electrodes. The spark leaves a small nucleus of flame that propagates into the unburnt gas. Until the nucleus is of the same order of 精品资料 - - - 欢迎下载 - - - - - - - - - - - 欢
8、迎下载 名师归纳 - - - - - - - - - -第 1 页,共 7 页 - - - - - - - - - - size as the turbulence scale, the flame propagation cannot be enhanced by the turbulence.1. Delay periodfrom A to B (first stage)This early burn period comprises the initial laminar combustion, and the transition to fully turbulent combusti
9、on, and is sometimes referred to as the delay period . The delay period is of approximately constant time duration. Figure compares the pressure diagrams for the cases when a mixture is ignited and when it is not ignited. The point at which the pressure traces diverge is ill-defined, but it is used
10、to denote the end of the delay period. The delay period is typically of 1-2 ms duration, and this corresponds to 15-30of crank angle at 2500 rpm. The early burn period depends on the temperature, pressure and composition of the fuel/air mixture, but it is a minimum for slightly richer than stoichiom
11、etric mixtures, in other words, when the laminar flame speed is highest. 2. Second stage (fast combustion) -from B to C The end of the second stage of combustion is also ill-defined on the pressure diagram, but occurs shortly after the peak pressure. The second stage of combustion is affected in the
12、 same way as the early burn period, and also by the turbulence. This is very fortunate since turbulence increases as the engine speed increases, and the time for the second stage of combustion reduces almost in proportion. In other words, the second stage of combustion occupies an approximately 精品资料
13、 - - - 欢迎下载 - - - - - - - - - - - 欢迎下载 名师归纳 - - - - - - - - - -第 2 页,共 7 页 - - - - - - - - - - constant number of crank angle degrees. In practice, the maximum cylinder pressure usually occurs 5-20 degree after top dead centre. We call this period fast combustion period. The mixture burns fiercely,
14、we use p MPa(o)to evaluate the pressure rise rate, and p is normally between 0.200.40 MPa/( o) 3. The final stage-after C The final stage of combustion is one in which the flame front is contacting more of the combustion chamber, with a reduced flame front area in contact with the unburned mixture,
15、the remaining unburned mixture in the combustion chamber being burnt more slowly. The cylinder pressure should also be falling, so unburned mixture will be leaving crevices. This final stage of combustion is very slow, and will not be complete by the time the exhaust valve opens. 4.2.2 Flame front p
16、ropagation in engines In the normal combustion, the forward boundary of the reacting zone is called the flame front. The motion of a mixture confined in a chamber of constant volume is complicated by the fact that expansion of the burned gases compresses the unburned part of the charge. It is the su
17、m of two movements: the rate at which the flame moves into the unburned portion of the charge, called the burning velocity, and the rate at which the flame front is pushed forward by the burned gases, called the transport velocity. The burning velocity of laminar flame is: mLLFvdtdmWhere m is the ma
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