Internal Combustion Engines

Internal Combustion Engines
Faculty - Er. Ashis Saxena

Index Unit 1 Unit 2 Unit 3 Unit 4 Unit 5 Introduction to I.C Engines
Fuels Unit 2 SI Engines Unit 3 CI Engines Unit 4 Engine Cooling Lubrication Supercharging Testing and Performance Unit 5 Compressors

Unit - 3 Chapter – 3 CI Engines

Injection System Difference between the Carburation and Injection
For the compression ignition engine, it is very important to promote a means of injecting fuel into the cylinder at the proper time in the cycle. This is so because the injection system starts and controls the combustion process. Difference between the Carburation and Injection Basically, the purpose of carburetion and fuel-injection is the same viz., preparation of the combustible charge. But in case of carburetion fuel is atomized by processes relying on the air speed greater than fuel speed at the fuel nozzle, whereas, in fuel-injection the fuel speed at the point of delivery is greater than the air speed to atomize the fuel. In carburetors, air flowing through a venturi picks up fuel from a nozzle located there. The amount of fuel drawn into the engine depends upon the air velocity in the venturi. In a fuel-injection system, the amount of fuel delivered into the air stream going to the engine is controlled by a pump which forces the fuel under pressure.

Injection Process When the fuel is injected into the combustion chamber towards the end of compression stroke, it is atomized into very fine droplets. These droplets vaporize due to heat transfer from the compressed air and form a fuel- air mixture. Due to continued heat transfer from hot air to the fuel, the Temperature reaches a value higher than its self-ignition temperature. This causes the fuel to ignite spontaneously initiating the combustion process.

Objectives of an Injection System
The injection system of the compression ignition engine should fulfill the following objectives consistently and precisely: Introduction of the fuel into the combustion chamber should take place within a precisely defined period of the cycle. The metering of amount of fuel injected per cycle should done very accurately. The quantities of fuel metered should vary to meet the changing load & speed requirements. The injection rate should be such that it results in the desired heat-release pattern. The injected fuel must be broken into very fine droplets. Proper spray pattern to ensure rapid mixing of fuel & air. Beginning & end of injection should be sharp. Timing the injection of the fuel correctly in cycle so that maximum power is obtained, ensuring economy & clean burning. Uniform distribution of fuel droplets throughout the combustion chamber.

Parts of an Injection System
To accomplish these objectives, a number of functional elements are required. These constitute together, the fuel injection system of the engine. These elements are as follows. Pumping elements to transfer the fuel from the tank to the cylinder, along with the associate piping and hardware. Metering elements to measure and supply the fuel at the rate as desired by the speed and load conditions prevailing. Metering controls to adjust the rate of the metering elements for changes in load and speed of the engine. Distributing elements to divide the metered fuel equally among the cylinders in a multi cylinder engine. Timing controls to adjust the start and stop of injection. Mixing elements to atomize and distribute the fuel within the combustion chamber

Fuel Injection Systems
There are two main classifications for fuel-injection systems, namely Air injection System: Solid (or airless) injection systems.

Air injection System In this method fuel is forced into the cylinder by means of compressed air to a very high pressure. The rate of fuel admission can be controlled by varying the pressure of air. The fuel is metered & pumped to the fuel valve by a camshaft driven fuel pump. The fuel valve is opened by means of a mechanical linkage operated by the camshaft which controls the timing of injection. The fuel valve is also connected to a high pressure air line fed by a multi stage compressor which supplies air at a pressure of about 60 to 70 bar.

Air injection System Advantages:
It provides better atomization & distribution of fuel. Heavy & viscous fuels, which are cheaper can also be injected. Disadvantages: This method is not used now a day due to following reasons: It requires a high pressure multi stage compression. A separate mechanical linkage is required to time the operation of fuel valve. The fuel valve sealing requires considerable skill. Due to the compression & the linkage the bulk of the engine increases. This also results in reduced B.P due to power loss in operating the compression & linkage. In case of sticking of the fuel valve, the system becomes quite dangerous due to the presence of high pressure air.

Solid (or airless) injection systems
In this system the liquid fuel is injected directly into the combustion chamber without, the aid of compressed air. Hence, it is also called airless injection or solid injection system. Solid injection systems can be classified into four types. Individual pump and nozzle system Unit injector system Common rail system Distributor system

Fuel Injection Systems
All the above systems comprise mainly of the following components. Fuel tank, Fuel feed pump to supply fuel from the main fuel tank to the injection system, Injection pump to meter and pressurize the fuel for injection, Governor to ensure that the amount of fuel injected is in accordance with variation in load, Injector to take the fuel from the pump and distribute it in the combustion chamber by atomizing it into fine droplets, Fuel filters to prevent dust and abrasive particles from entering the pump and injectors thereby minimizing the wear and tear of the components.

A typical Solid Injection System
Pressure relief valve

A typical Solid Injection System
A typical arrangement of various components for the solid injection system used in a Cl engine is shown in Fig. Fuel from the fuel tank first enters the coarse filter from which is drawn into the plunger feed pump where the pressure is raised very slightly. Then the fuel enters the fine filter where all the dust and dirt particles are removed. From the fine filter the fuel enters the fuel pump where it is pressurized to about 200 bar and injected into the engine cylinder by means of the injector. Any spill over in the injector is returned to the fine filter. A pressure relief valve is also provided for the safety of the system. The above functions are achieved with the components listed above.

Individual Pump and Nozzle System
In this system, each cylinder is provided with one pump and an injector. In this arrangement a separate metering and compression pump is provided for each cylinder. The pump may be placed close to the cylinder as shown in Fig. (a) or,

Individual Pump and Nozzle System
They may be arranged in a cluster as shown in Fig. (b). The high pressure pump plunger is actuated by a cam, and produces the fuel pressure necessary to open the injector valve at the correct time. The amount of fuel injected depends on the effective stroke of the plunger.

Unit Injector System The unit injector system, is one in which the pump and the injector nozzle are combined in one housing. Each cylinder is provided with one of these unit injectors.

Unit Injector System Fuel is brought up to the injector by a low pressure pump, where at the proper time, a rocker arm actuates the plunger and thus injects the fuel into the cylinder. The amount of fuel injected is regulated by the effective stroke of the plunger. The pump and the injector can be integrated in one unit.

Common Rail System In the common rail system, a HP pump supplies fuel, under high pressure, to a fuel header. High pressure in the header forces the fuel to each of the nozzles located in the cylinders.

Common Rail System At the proper time, a mechanically operated (by means of a push rod and rocker arm) valve allows the fuel to enter the proper cylinder through the nozzle.

Common Rail System The pressure in the fuel header must be that, for which the injector system was designed, i.e., it must enable to penetrate and disperse the fuel in the combustion chamber. The amount of fuel entering the cylinder is regulated by varying the length of the push rod stroke. A high pressure pump is used for supplying fuel to a header, from where the fuel is metered by injectors (assigned one per cylinder).

Common Rail System

Distributor System In this system the pump which pressurizes the fuel also meters and times it. The fuel pump after metering the required amount of fuel supplies it to a rotating distributor at the correct time for supply to each cylinder. The number of Injection strokes per cycle for the pump is equal to the number of cylinders. Since there is one metering element in each pump, a uniform distribution is automatically ensured. Not only that, the cost of the fuel-injection system also reduces to a value less than two-thirds of that for individual pump system.

Distributor System

Comparison of Solid Injection Systems
Comparison of Various Fuel-injection Systems Job Air injection system Solid injection system Individual pump Common rail Distributor Metering Timing Injection rate Atomization Distribution Pump Fuel cam Spray valve Pump cam Spray tip Injection valve

Fuel feed pump Fig shows fuel feed pump which is of spring loaded plunger type. The plunger is actuated through a push rod from the cam shaft. At the minimum lift position of the cam the spring force on the plunger creates a suction which causes fuel flow from the main tank into the pump.

Fuel feed pump When the cam is turned to its maximum lift position, the plunger is lifted upwards. At the same time the inlet valve is closed and the fuel is forced through the outlet valve.

Fuel feed pump When the operating pressure gets released, the plunger return spring ceases to function resulting in varying of the pumping stroke under varying engine loads according to the quantity of fuel required by the injection pump.

Injection pump The main objectives of fuel-injection pump is to deliver accurately metered quantity of fuel under high pressure (in the range from 120 to 200 bar) at the correct instant to the injector fitted on each cylinder. Injection pumps are of two types. Jerk type pumps Distributor type pump

Jerk Type Pump It consists of a reciprocating plunger inside a barrel.
The plunger is driven by a camshaft. The working principle of jerk pump is illustrated in Fig. A sketch of a typical plunger is shown. a

Jerk Type Pump A schematic diagram of the plunger within the barrel is shown. Near the port A, fuel is always available under relatively low pressure. While the axial movement of the plunger is through cam shaft, its rotational movement about its axis by means of rack D. Port B is the orifice through which fuel is delivered to the injector. At this stage it. is closed by means of a spring loaded check valve. b

Jerk Type Pump When the plunger is below port A. the fuel gets filled in the barrel above it. As the plunger rises and closes the port A the fuel will flow out through port C. This is because it has to overcome the spring force of the check valve in order to flow through port B. Hence it takes the easier way out. via port C.

Jerk Type Pump At this stage rack rotates the plunger and as a result port C also closes. The only escape route for the fuel is past the check valve through orifice B to the injector. This is the beginning of injection and also the effective stroke of the plunger. c d

Jerk Type Pump The injection continues till the helical indentation on the plunger uncovers port C. Now the fuel will take the easy way out through C and the check valve will close the orifice B. The fuel injection stops and the effective stroke ends. Hence the effective stroke of the plunger is the axial distance traversed between the time port A is closed off and the time port C is uncovered. c d

Jerk Type Pump & (f) The plunger is rotated to the position shown. The same sequence of events occur. But in this case port C is uncovered sooner. Hence the effective stroke is shortened. e f

Jerk Type Pump It is important to remember here that though the axial distance traversed by the plunger is same for every stroke, the rotation of the plunger by the rack determining the length of the effective stroke and thus the quantity of fuel injected. A typical example of this type of pump is the Bosch fuel-injection pump shown in Fig. below.

Diagram illustrating an Actual Method of Controlling Quantity of Fuel Injected in a CI engine.

Distributor Type Pump This pump has only a single pumping element and the fuel is distributed to each cylinder by means of a rotor. There is a central longitudinal passage in the rotor and also two sets of radial holes (each equal to the number of engine cylinders) located at different heights. One set is connected to pump via central passage whereas the second set is connected to delivery lines leading to injectors of the various cylinders.

Distributor Type Pump The fuel is drawn into the central rotor passage from the inlet port when the pump plunger move away from each other. Wherever, the radial delivery passage in the rotor coincides with the delivery port for any cylinder the fuel is delivered to each cylinder in turn. Main advantages of this type of pump lies in its small size and its light weight. A schematic diagram Roosa Master distributor pump is shown in Fig. below.

Electronic fuel injection system
Modern gasoline injection system use engine sensors, a computer and solenoid operated fuel injectors to meter & inject the right amount of fuel into the engine cylinder. These system is called as electronic fuel injection system(EFL) use electrical & electronic devices to monitor & control engine operation. An electronic control unit (ECU) or computer receives electrical signals in the form of current or voltage from various sensors.

It then uses the stored data to operate the injectors , ignition system & other engine related devices. As a result, less unburned fuel leaves the engine as emissions & the vehicle gives better mileage. Under full load, the ECU will sense a wide open throttle, high intake manifold pressure,& high inlet air flow. The ECU will then increase the injector pulse width to enrich the mixture which will enable the engine to produce higher power.

Under low load & idling conditions, the ECU will shorten the pulse width by which the injectors are kept in the closed position over a longer period of time. Because of this, air-fuel mixture will become leaner & will result in better fuel economy. EFI system has a cold start injector too.

This is an extra injector that sprays fuel into the center of the engine intake manifold when the engine is cold. It serves the same purpose as the carburetor choke. The cold start injector ensures easy engine start up in very cold weather.

Sensors used in EFI system
Exhaust gas (or) oxygen sensor. Engine temperature sensor. Air flow sensor. Air inlet temperature sensor. Throttle position sensor. Manifold pressure sensor. Camshaft position sensor. Knock sensor.

Advantages Better atomization & vaporization will make the engine less knock. Manifold wetting is eliminated due to the fuel being injected into or close to cylinder & need not flow through the manifold. Atomization of fuel is independent of cranking speed & therefore starting will be easier. Distribution of fuel being independent of vaporization less volatile fuel can be used. Position of the injection unit is not so critical & thereby the height of the engine can be less. Disadvantages High maintenance cost. Difficulty in servicing. Possibility of malfunction of some sensors.

Injection Timing Consider a cylinder of a four cylinder engine.
The fuel is injected into the inlet manifold of each cylinder at different timings. The timing at which the injection of the fuel takes place inside the inlet manifold is called injection timing. Below is the injection timing for one cylinder of this four cylinder engine. In one cylinder, the piston moves up from the BDC to TDC during the exhaust stroke.

Injection Timing Just before the piston reached TDC during this exhaust stroke, injection of fuel takes place into the inlet manifold of this cylinder at about 60 crank angle before TDC. This injected fuel mixes with the air intake chamber. Thus the air fuel mixture is obtained. At the beginning of the suction stroke, intake valve opens and the air fuel mixture is sucked into the cylinder during the suction stroke. According to the firing order, the injection of the fuel takes place inside the inlet manifolds of the other three cylinders at various timings.

Injection Timing In this four cylinder engine, the ECU calculates the approximate injection timing for each cylinder and the air fuel mixture is made available at each suction stroke. In order to meet the operating conditions, the injection valve is kept open for a longer time by ECU. For ex, if the vehicle is accelerating, the injection valve will be opened for a longer time, in order to supply additional fuel to the engine.

Scavenging In automotive usage, scavenging is the process of pushing exhausted gas-charge out of the cylinder or the process of removing burnt gases, from the combustion chamber of the engine cylinder, is known a scavenging. The last stroke of an IC engine is the exhaust, which means the removal of burnt gases from the engine cylinder. It has been experienced that the burnt gases in the engine cylinder are not completely exhausted before the suction stroke but a part of the gases still remain inside the cylinder and mix with the fresh charge. As a result of this mixing, the fresh charge gets diluted and its strength is reduced.

Scavenging in 2 & 4 stroke engines
Four-stroke cycle engines: In a four stroke cycle engine, the scavenging is very effective as the piston during the exhaust stroke pushes out the burnt gases from the engine cylinder. It may be noted that a small quantity of burnt gases remain in the engine cylinder in the clearance space. Two-stroke cycle engine: In a two-stroke cycle engine, the scavenging is less effective as the exhaust port is open for a small fraction of the crank revolution. Moreover, as the transfer and exhaust port are open simultaneously during a part of the crank revolution, therefore fresh charge also escapes out along with the burnt gases. This difficulty is overcome by designing the piston crown of a particular shape.

Types of Scavenging 1. Cross flow scavenging: In this method, the transfer port (or inlet port for the engine cylinder) and exhaust port are situated on the opposite sides of the engine cylinder (as is done in case of two-stroke cycle engines). The piston crown is designed into a particular shape, so that the fresh charge moves upwards and pushes out the burnt gases in the form of cross flow as. Shown in (a).

Types of Scavenging 2. Backflow or loop scavenging: In this method, the inlet and outlet ports are situated on the same side of the engine cylinder. The fresh charge, while entering into the engine cylinder, forms a loop and pushes out the burnt gases as shown in (b).

Types of Scavenging 3. Uniflow scavenging: In this method, the fresh charge, while entering from one side (sometimes two sides) of the engine cylinder pushes out the gases through the exit valve situated on the top of the cylinder. In uniflow scavenging, both the fresh charge and burnt gases move in the same upward direction.

Combustion in CI engines Versus in SI Engine
In the SI engine, a homogeneous carbureted mixture of gasoline vapor and air, in a certain proportion, is compressed and the mixture is ignited at one place before the end of the compression stroke by means of an electric spark. A single flame front progresses through the air-fuel mixture after ignition.

In the Cl engine, only air is compressed through a high compression ratio raising its temperature and pressure to a high value. Fuel is injected through one or more jets into this highly compressed air in the combustion chamber. Here, the fuel jet disintegrates into a core of fuel surrounded by a spray envelope of air and fuel particles [Fig(a)].

This spray envelope is created both by the atomization and vaporization of the fuel. The turbulence of the air in the combustion chamber passing across the jet tears the fuel particles from the core. A mixture of air and fuel forms at some location in the spray envelope and oxidation starts.

The liquid fuel droplets evaporate by absorbing the latent heat of vaporization from the surrounding air which reduces the temperature of a thin layer of air surrounding the droplet and some time elapses before this temperature can be raised again by absorbing heat from the bulk of air. As soon as this vapor and the air reach the level of the auto-ignition temperature and if the local A/F ratio is within the combustible range, ignition takes place. Thus, it is obvious that at first there is a certain delay period before ignition takes place.

Since the fuel droplets cannot be injected and distributed uniformly throughout the combustion space, the fuel-air mixture is essentially heterogeneous. If the air within the cylinder were motionless under these conditions there will not be enough oxygen in the burning zone and burning of the fuel would be either slow or totally fail as it would be surrounded by its own products of combustion [Fig. (b)].

Hence, an orderly and controlled movement must be imparted to the air and the fuel so that a continuous flow of fresh air is brought to each burning droplet and the products of combustion are swept, away. This air motion is called the air swirl and its effect is shown in Fig. (c).

In an SI engine, the turbulence is a disorderly air motion with no general direction of flow. However, the swirl which is required in CI engines, is an orderly movement of the whole body of air with a particular direction of flow and it assists the breaking up of the fuel jet. Intermixing of the burned and unburned portions of the mixture also takes place due to this swirl.

In the SI engine, the ignition occurs at one point with a slow rise in pressure whereas in the Cl engine, the ignition occurs at many points simultaneously with consequent rapid rise in pressure. In contrast to the process of combustion in SI engines, there is no definite flame front in CI engines.

In an SI engine, the air-fuel ratio remains close to stoichiometric from no load to full load. But in a Cl engine, irrespective of load, at any given speed, an approximately constant supply of air enters the cylinder. With change in load, the quantity of fuel injected is changed, varying the air-fuel ratio. The overall air-fuel ratio thus varies from about 18:1 at full load to about 80:1 at no load. It is the main aim of the Cl engine designer that the A/F ratio should be as close to stoichiometric as possible while operating at full load since the mean effective pressure and power output are maximum at that condition.

Thermodynamic analysis of the engine cycles has clearly established that operating an engine with a leaner air-fuel ratio gives a better thermal efficiency but the mean effective pressure and the power output reduce. Therefore, the engine size becomes bigger for a given output if it is operated near the stoichiometric conditions, the A/F ratio in certain regions within the chamber is likely to be so rich that some of the fuel molecules will not be able to find the necessary oxygen for combustion and thus produce a noticeably black smoke. Hence the CI engine is always designed to operate with an excess air, of 15% to 40% depending upon the application.

Stages of combustion in CI engines
The combustion in a Cl engine is considered to be taking place in four stages. It is divided into The ignition delay period, The period of rapid combustion, The period of controlled combustion The period of after-burning.

Stages of combustion in CI engines : Ignition Delay
Ignition Delay Period The ignition delay period is also called the preparatory phase during which some fuel has already been admitted but has not yet ignited. This period is counted from the start of injection to the point where the pressure-time curve separates from the motoring curve indicated as start of combustion in Fig. The fuel does not ignite immediately upon injection into the combustion chamber. There is a definite period of inactivity between the time when the first droplet of fuel hits the hot air in the combustion chamber and the time it starts through the actual burning phase. This period is known as the ignition delay period.

The ignition delay period can be divided into two parts, the physical delay & the chemical delay. Physical Delay: The physical delay is the time between the beginning of injection and the attainment of chemical reaction conditions. During this period, the fuel is atomized, vaporized, mixed with air and raised to its self ignition temperature. This physical delay depends on the type of fuel, for light fuel the physical delay is small while for heavy viscous fuels the physical delay is high. The physical delay is greatly reduced by using high injection pressures, higher combustion chamber temperatures and high turbulence to facilitate breakup of the jet and improving evaporation.

Chemical Delay: During the chemical delay, reactions start slowly and then accelerate until inflammation or ignition takes place. Generally, the chemical delay is larger than the physical delay. However, it depends on the temperature of the surroundings and at high temperatures, the chemical reactions are faster and the physical delay becomes longer than the chemical delay.

Stages of combustion in CI engines : Period of Rapid Combustion
The period of rapid combustion also called the uncontrolled combustion, is that phase in which the pressure rise is rapid. During the delay period, the droplets have had time to spread over a wide area and fresh air is always available around the droplets. Most of the fuel admitted would have evaporated and formed a combustible mixture with air. By this time, the preflame reactions would have also been completed.

Stages of combustion in CI engines : Period of Rapid Combustion
The period of rapid combustion is counted from end of delay period or the beginning of the combustion to the point of maximum pressure on the indicator diagram. The rate of heat-release is maximum during this period. It may be noted that the pressure reached during the period of rapid combustion will depend on the duration of the delay period (the longer the delay the more rapid and higher is the pressure rise since more fuel would have accumulated in the cylinder during the delay period).

Stages of combustion in CI engines : Period of Controlled Combustion
The rapid combustion period is followed by the third stage, the controlled combustion. The temperature and pressure in the second stage is already quite high. Hence the fuel droplets injected during the second stage burn faster with reduced ignition delay as soon as they find the necessary oxygen and any further pressure rise is controlled by the injection rate. The period of controlled combustion is assumed to end at maximum cycle temperature.

Stages of combustion in CI engines : Period of Controlled Combustion
Period of After-Burning Combustion does not cease with the completion of the injection process. The unburnt and partially burnt fuel particles left in the combustion chamber start burning as soon as they come into contact with the oxygen. This process continues for a certain duration called the after-burning period. Usually this period starts from the point of maximum cycle temperature and continues over a part of the expansion stroke. Rate of after-burning depends on the velocity of diffusion and turbulent mixing of unburnt and partially burnt fuel with the air. The duration of the after-burning phase may correspond to degrees of crank travel from TDC.

Block Diagram illustrating the Combustion Process in a Cl Engine

Phenomenon of knock in CI engines
In CI engines the injection process takes place over a definite interval of time. Consequently, as first few droplets to be injected are passing through the ignition delay period, additional droplets are being injected into the chamber. If the ignition delay of the fuel being injected is short, the first few droplets will commence the actual burning phase in a relatively short time after injection and a relatively small amount of fuel will be accumulated in the chamber when actual burning commences. As a result, the mass rate of mixture burned will be such as to produce a rate of pressure rise that will exert a smooth force on the piston, as shown in Fig. (a).

If, on the other hand, the ignition delay is longer, the actual burning of the first few droplets is delayed and a greater quantity of fuel droplets gets accumulated in the chamber. When the actual burning commences, the additional fuel can cause too rapid a rate of pressure rise as shown in Fig. (b), resulting in a jamming of forces against the piston and rough engine operation.

If the ignition delay is quite long, so much fuel can accumulate that the rate of pressure rise is almost instantaneous, as shown in Fig (c).

Such a situation produces the extreme pressure differentials and violent gas vibrations known as knocking and is evidenced by audible knock. The phenomenon is similar to that in the SI engine. However, in the SI engine, knocking occurs near the end of combustion whereas in the Cl engine, knocking occurs near the beginning of combustion. In order to decrease the tendency of knock it is necessary to start the actual burning as early as possible after the injection begins. In other words, it is necessary to decrease the ignition delay and thus decrease the amount of fuel present when the actual burning of the first few droplets start.

Combustion chamber design
The most important function of the Cl engine combustion chamber is to provide proper mixing of fuel and air in a short time. In order to achieve this, an organized air movement called the air swirl is provided to produce high relative velocity between the fuel droplets and the air. The fuel is injected into the combustion chamber by an injector having a single or multiple orifices. The increase in the number of jets reduces the intensity of air swirl needed.

When the liquid fuel is injected into the combustion chamber, the spray cone gets disturbed due to the air motion and turbulence inside. The onset of combustion will cause an added turbulence that can be guided by the shape of the combustion chamber. CI engine combustion chambers are classified into two categories: Direct-Injection (Dl) Type: This type of combustion chamber is also called an open combustion chamber. In this type the entire volume of the combustion chamber is located in the main cylinder and the fuel is injected into this volume.

Indirect-Injection (IDI) Type: In this type of combustion chambers, the combustion space is divided into two parts, one part in the main cylinder and the other part in the cylinder head. The fuel-injection is effected usually into that part of the chamber located in the cylinder head. These chambers are classified further into: Swirl chamber in which compression swirl is generated. Pre-combustion chamber in which combustion swirl is induced! Air cell chamber in which both compression and combustion swirl are induced.

Direct - lnjection Chambers
An open combustion chamber is defined as one in which the combustion space is essentially a single cavity with little restriction from one part of the chamber to the other and hence with no large difference in pressure between parts of the chamber during the combustion process. In four-stroke engines with open combustion chambers, induction swirl is obtained either by careful formation of the air intake passages or by masking a portion of the circumference of the inlet valve whereas in two stroke engines it is created by suitable form for the inlet ports. These chambers mainly consist of space formed between a flat cylinder head and a cavity in the piston crown in different shapes. The fuel is injected directly into this space. The injector nozzles used for this type of chamber are generally of multihole type working at a relatively high pressure (about 200 bar).

Direct - lnjection Chambers
The main advantages of this type of chambers are: Minimum heat loss during compression because of lower surface area to volume ratio and hence, better efficiency. No cold starting problems. Fine atomization because of multihole nozzle. The drawbacks of these combustion chambers are: High fuel-injection pressure required and hence complex design of fuel-injection pump. Necessity of accurate metering of fuel by the injection system particularly for small engines.

Direct - lnjection Chambers - Types
Shallow Depth Chamber: In shallow depth chamber the depth of the cavity provided in the piston is quite small. This chamber [Fig. (a)] is usually adopted for large engines running at low speeds. Since the cavity diameter is very large, the squish is negligible.

Hemispherical Chamber: This chamber [Fig. (b)] also gives small squish. However, the depth to diameter ratio for a cylindrical chamber can be varied to give any desired squish to give better performance.

Cylindrical Chamber: This design [Fig. (c)] was attempted in recent diesel engines. This is a modification of the cylindrical chamber in the form of a truncated cone with base angle of 30°. The swirl was produced by masking the valve for nearly 180° of circumference. Squish can also be by varying the depth.

Toroidal Chamber: The idea behind this shape [Fig. (d)] is to provide a powerful squish along with the air movement, similar to that of the familiar smoke ring, within the toroidal chamber. Due to powerful squish the mask needed on inlet valve is small and there is better utilization of oxygen. The cone angle of spray for this type of chamber is 150° to 160°.

Indirect - lnjection Chambers
A divided combustion chamber is defined as one in which the combustion space is divided into two or more distinct compartments connected by restricted passages. This creates considerable pressure differences between them during the combustion process.

Indirect - lnjection Chambers - Types
Swirl Chamber: Swirl chamber consists of a spherical-shaped chamber separated from the engine cylinder and located in the cylinder head. Into this chamber, about 50% of the air is transferred during the compression stroke. A throat connects the chamber to the cylinder which enters the chamber in a tangential direction so that the air coming into this chamber is given a strong rotary movement inside the swirl chamber and after combustion, the products rush back into the cylinder through the same throat at much higher velocity.

This causes considerable heat loss to the walls of the passage which can be reduced by employing a heat-insulated chamber. However, in this type of combustion chambers even with a heat insulated passage, the heat loss is greater than that in an open combustion chamber which employs induction swirl. This type of combustion chamber finds application where fuel quality is difficult to control, where reliability under adverse conditions is more important than fuel economy. The use of single hole of larger diameter for the fuel spray nozzle is often important consideration for the choice of swirl chamber engine.

Precombustion Chamber: A typical precombustion chamber consists of an antichamber connected to the main chamber through a number of small holes (compared to a relatively large passage in the swirl chamber). The precombustion chamber is located in the cylinder head and its volume accounts for about 40% of the total combustion space. During the compression stroke the piston forces the air into the precombuhtion chamber. The fuel is injected into the prechamber and the combustion is initiated.

The resulting pressure rise forces the flaming droplets together with some air and their combustion products to rush out into the main cylinder at high velocity through the small holes. Thus it creates both strong secondary turbulence and distributes the flaming fuel droplets throughout the air in the main combustion chamber where bulk of combustion takes place. About 80% of energy is released in main combustion chamber.

The rate of pressure rise and the maximum pressure is lower compared to those of open type chamber. The initial shock of combustion is limited to precombustion chamber only. The precombustion chamber has multi-fuel capability without any modification in the injection system because of the temperature of prechamber. The variation in the optimum injection timing for petrol and diesel operations is only 2° for this chamber compared to 8° to 10° in the other designs.

Air-Cell Chamber: In this chamber, the clearance volume is divided into two parts, one in the main cylinder and the other called the energy cell. The energy cell is divided into two parts, major and minor, which are separated from each other and from the main chamber by narrow orifices. A pintle type of nozzle injects the fuel across the main combustion chamber space towards the open neck of the air cell. During compression, the pressure in the main chamber is higher than that Inside the energy cell due to restricted passage area between the two.

At the TDC the difference in pressure will be high and air will be forced at high velocity through the opening into the energy cell and this moment the fuel-injection also begins. Combustion starts initially in the main chamber where the temperature is comparatively higher but the rate of burning is very slow due to absence of any air motion. In the energy cell, the fuel is well mixed with air and high pressure is developed due to heat release & the hot burning gases blow out through the small passage into the main chamber. This high velocity jet produces swirling motion in the main chamber and thereby thoroughly mixes the fuel with air resulting in complete combustion.

Internal Combustion Engines

Similar presentations

Presentation on theme: "Internal Combustion Engines"— Presentation transcript:

Similar presentations

About project

Feedback

Log in

Auth with social network:

Internal Combustion Engines

Similar presentations

Presentation on theme: "Internal Combustion Engines"— Presentation transcript:

Similar presentations

About project

Feedback