《发动机原理》双语教案

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机械毕业设计英文外文翻译144发动机工作原理 - 副本

机械毕业设计英文外文翻译144发动机工作原理 - 副本

Engine Operating PrinciplesMost automobile engines are internal combustion,reciprocating 4-stroke gasoline engines,but other types have been used,including the diesel,the rotary(wankel),the 2-srtoke,and stratified charge.Reciprocating means up and dowm or banck and forth ,It is the up and down action of a piston in the cylinder blick,or engine block.The bilck is an iron or aluminum casting that contains engine cylinders and passges called water jackets for coolant circulation.The top of the block is convered with the cylinder head.Which forms the combustion chanber.The bottom of the block is covered with an oil pan or oil sump.Power ia produced by the linear motion of a piston in a cylinder.However,this linear motion must be changed into rotary motion to turn the wheels of cars of trucks.The piston is attached to the top of a connecting rod by a pin ,called a piston pin or wrist pin.The bottom of the connecting rod is attached to the crankshaft.The connecting rod transmits the up-and-down motion of the piston to the crankshaft,which changes it into rotary motion.Term: stroke is used to indicate the movement within thecylinder piston, piston stroke is the distance from the engine type according to need two-stroke or four-stroke cycle to finish a job and four stroke engines are also called otto engine, in order to commemorate German engineers otto, he is the first application in 1876, the principle of in four stroke engines, cylinder piston required to complete a four-stroke cycle, each stroke work according to their behavior named respectively: intake stroke, compression stroke, function and exhaust stroke.1. Intake strokeWhen the piston moves down, spray the mixture through open after entering the inlet valve, in order to achieve maximum cylinder amount of inlet in Detroit, arrive before BDC 10 °, open and exhaust has 20 ° to open the inlet valve overlap, has been opened to the pistons to come fully into the mixture after about 50 °.2. Compression strokeThe piston start moving up huge inlet valve closed, and the mixture in the combustion chamber, according to the different factors including compression compression ratio, the throttle valve, pressure revs up to about 1 mpa, close to the top, the spark plug stroke produces the spark gap in the breakdown ignition mixture lighting.3. Doing workBurning gas pressure of inflation rose to 3.5 mpa, promote the piston moves to the cylinder, and exhaust door open.4 gas strokeWith exhaust before more open about 50 °, piston, make up in the air pressure drops in exhaust stroke, reduce backpressure, discharge waste piston stroke, for the next intake, normally, inlet in exhaust before opening.Only the engine keep running, each cylinder within four four-stroke cycle continuously.Two stroke engine also through the four-stroke cycle to complete a job but intake stroke, compression stroke for a stroke, do work schedule another stroke, the four-stroke cycle and two terms two travel itinerary is called the term two-cycle but actually not so accurate. However,the intake and the compression actions are combined in one seroke,and the power and exhaust actions are combined in the other stroke.The term 2-stroke cyde or 2-stroke is preferred to the term 2-cyde,which is really not accurate.In automobile engines,all pistons are attached to a single crankshaft.the more cylinders an engine has,the more power strokes produced for cach revolution.This means that an 8-cylinder engine runs more smoothly bacause the poweratrokes are closer togther in time and in degrees of engine rotation.The cylinders of multi-cylinder automotive engines arranged in one of three ways.1.Inline engines use a single block of cylinder.Most 4-cylinder and any 6-cylinder engines are of this design.The cylinders do not have to be vertical.They can be inclined either side.2.V-type engines use two equal bands of cylinders,usually inclined 60 degrees or 90 degrees from the cach other.Most V-type engines have 6 or 8 cylinders,although v-4 and v-12 engines have been built.3.Horizontally opposed,or pancake engines have two equal banks of cylinders 180 degrees apart.These space saving engine designs are often air-cooled,and are found in the Chevrolet Carvair,Porsches,Subaus,and Volkswagens.Subaus design is liquid cooled.are often air-cooled,and are found in the Chevrolet Carvair,Porsches,Subaus,and Volkswagens.Subaus design is liquid te-model Volkswagen vans use a liquid-cooled version of the air cooled VWhorizontally opposed engine.发动机工作原理大多数汽车的发动机是内燃机,往复四冲程汽油机,但是也有使用其它类型的发动机,包括柴油机,转子发动机,二冲程发动机和分成燃烧发动机。

汽车专业英语教案

汽车专业英语教案

汽车专业英语教案章节一:汽车行业概述教学目标:1. 了解汽车行业的发展历程和现状。

2. 掌握汽车行业的主要领域和趋势。

3. 提高听力理解能力和口语表达能力。

教学内容:1. 汽车行业的发展历程。

2. 汽车行业的现状和挑战。

3. 汽车行业的主要领域和趋势。

教学活动:1. 观看汽车行业发展历程的短片。

2. 分组讨论汽车行业的现状和挑战。

3. 角色扮演,模拟汽车行业的未来趋势。

章节二:汽车发动机原理教学目标:1. 了解汽车发动机的基本原理和工作过程。

2. 掌握汽车发动机的主要部件和功能。

3. 提高听力理解能力和口语表达能力。

教学内容:1. 汽车发动机的基本原理。

2. 汽车发动机的工作过程。

3. 汽车发动机的主要部件和功能。

教学活动:1. 观看汽车发动机工作原理的演示。

2. 分析汽车发动机的主要部件和功能。

3. 小组讨论,总结汽车发动机的工作过程。

章节三:汽车电气系统教学目标:1. 了解汽车电气系统的基本原理和组成。

2. 掌握汽车电气系统的主要部件和功能。

3. 提高听力理解能力和口语表达能力。

教学内容:1. 汽车电气系统的基本原理。

2. 汽车电气系统的组成和主要部件。

3. 汽车电气系统的工作过程和功能。

教学活动:1. 观看汽车电气系统工作原理的演示。

2. 分析汽车电气系统的主要部件和功能。

3. 小组讨论,总结汽车电气系统的工作过程。

章节四:汽车transmission 系统教学目标:1. 了解汽车transmission 系统的基本原理和类型。

2. 掌握汽车transmission 系统的主要部件和功能。

3. 提高听力理解能力和口语表达能力。

教学内容:1. 汽车transmission 系统的基本原理。

2. 汽车transmission 系统的类型和特点。

3. 汽车transmission 系统的主要部件和功能。

教学活动:1. 观看汽车transmission 系统工作原理的演示。

2. 分析汽车transmission 系统的主要部件和功能。

《发动机原理》双语教案(chapter 3)

《发动机原理》双语教案(chapter 3)

Chapter 3 Fuels and Chemical Thermodynamics Key: Using demands and characteristics of fuels, chemical thermodynamics mechanicals of fuels.Difficult points: Improve combustion mechanicals of fuels.3.1 Conventional fuels for internal combustionengineThe engine converts heat energy which is obtained from the chemical combination of the fuel with oxygen, into mechanical energy.The fuels most commonly used in internal combustion engines (gasoline or petrol, and diesel fuels) are blends of many different hydrocarbon compounds obtained by refining petroleum or crude oil.The differences in the physical and chemical property between the different types of hydrocarbon depend on their chemical composition and affect mainly the combustion processes and hence, the proportion of fuel and air required in the engine.3.1.1 Characteristics of petrol(gasoline)1. Antiknock performanceAbnormal burning or detonation in an SI engine combustion chamber causes a very high rate of energy release, excessive temperature and pressure inside the cylinder adversely affects its thermal efficiency. Therefore the characteristics of the fuel used should be such that it resists the tendency to produce detonation and this property is called its antiknock property.The octane number of a fuel is a measure of its antiknock performance. The octane requirement of an engine varies with compression ratio, geometrical and mechanical considerations, and also its operating conditions.There are two commonly used octane scales, research octane number (RON) and motor octane number(MON). The average of the two octane number rating methods,is known as the antiknock index; thus Antiknockindex=2RONMON.There are three specifications of gasoline in China: No. 90, No. 93 and No. 97, which is the value of respective research octane number.2. VolatilityVolatility is the process that compounds from solid or liquid into gas or steam. The usual practice of measuring the fuel volatility is the distillation of the fuel.The portion of the distillation below 10% is desirable for best starting and warm-up. However, high rate if vaporization of gasoline can set up a vapor lock in the fuel passages. 40 and 50% distillation temperature are used to assess the average rate of vaporization of gasoline. With higher 90% distillation temperature, there would be more residuals left after distillation.3.1.2 Characteristics of diesel fuelSelf-ignition: The most important characteristic of diesel fuel is the cetane number, as this indicates how readily the fuel self-ignites.Volatility: the process that compounds from solid or liquid into gas or steam. The usual practice of measuring the fuel volatility is the distillation of the fuel.Viscosity: the measure that fuel can flow through the fuel system. It may influent the quality of inject and spray.Specification of diesel fuel: When diesel engine is cooled, a point will be reached at which the highest molecular mass components will start to solidity and form a waxy precipitate. The temperature at which wax starts to dissolve out is referred to assolidifying temperature. There are the following specifications in automobile used light diesel fuel according to the solidifying temperature: 10,0,-10,-20,-35 and -50.Section 2 Alternative FuelsAlternative fuels: Refers to replace the conventional gasoline and diesel fuel for using in engine. Currently liquid and gaseous fuels are mainly using in engine.3.2.1 Liquid fuels1. AlcoholAlcohols are an attractive alternative fuel because they can be obtained from both natural and manufactured sources.The advantages of alcohol as a fuel are:(1) It can be obtained from a number of sources.(2)It is a high octane fuel with anti-knock index numbers of over 100.(3)It produces less overall emissions when compared with gasoline.The disadvantages of alcohol as a fuel are:(1)Alcohols have low energy content; the calorific value is almost the half.(2)Combustion of alcohols produces more aldehydes in the exhaust.(3)Alcohol is much more corrosive than gasoline on copper, brass, aluminum, rubber and many plastics.(4)It has poor cold weather starting characteristics due to low vapor pressure and evaporation.2. MethanolThe most common mixtures are M85(85% methanol and 15% gasoline ) and M10(10% methanol and 90% gasoline).3. EthanolTwo mixture combinations that are important are E85(ethanol) and E10(gasohol).3.2.2 Gaseous fuels1. HydrogenAdvantages: (1) Low emissions. (2) Fuel availability. (3) Fuel leakage to environment is not pollutant. (4) High energy content per volume when store as a liquid.Disadvantages: (1) Requirement of heavy, bulky fuel storage both in vehicle and at the service station. (2) Difficult to refuel. (3) Poor engine volumetric efficiency.2. Natural gasNatural gas obtained from oil wells is called casing head gas. The composition varies considerably from place to place and from time to time. It is stored as compressed natural gas(CNG) at pressures of 16 to 25 bar, or as liquefied petroleum gas (LPG) at pressures of 70 to 210 bar and a temperature around -160ºC.Advantages:(1) Octane number is around 120, which makes it a very good SI engine fuel.(2) Low engine emissions.(3) Fuel is fairly abundant worldwide.Disadvantages :(1) Low energy density resulting in low engine performance. (2) Low engine volumetric efficiency because it is a gaseous fuel. (3) Need for largepressurized fuel storage tank. (4) Inconsistent fuel properties. (5) Refueling is a slow process.3. BiogasThe biogas is generally produced from by dung from different beasts as cow, buffalo, goat, sheep, horse donkey, and elephant. Some other sources are: sewage, crop residue, vegetable waste, water hyacinth, alga, poultry droppings, pig manure and ocean kelp.Biogas is produce by digestion, pyrolysis or hydrogasification. The main combustible component in biogas is CH4and another component is CO2which reduces its octane number.The advantages of biogas are:(1) Biogas possesses excellent antilock properties with an equivalent octane number in excess of 120 compared with 87 for regular petrol.(2) Its auto-ignition temperature is higher than petrol.(3) Although its caloric value is lesser than petrol, it is possible to use higher compression ratio for the same size engine thus making it possible to generate the same amount of power.The advantages of using biogas as fuel in CI engine are:(1) A uniform gas-air mixture is available in multi-cylinder engine at all times.(2) Due to clean operation of the engine there is virtually no CO emission in exhaust.(3) When biogas is used as a fuel, NO X emissions are reduced by about60%.(4) Soot is virtually eliminated and exhaust is found less pungent odor than that obtained while operating the engine with diesel fuel.Attempts to use many other types of fuel have been tried throughout the history of internal combustion engines and will go on. Other possible fuels include: Producer Gas, Blast Furnace Gas, Coke Oven Gas, Benzol, Acetone and Diethyl Ether.Section 3 Combustion chemistryFollowing conditions are necessary for combustion to take place: (1) A combustion mixture. (2) Some means to initiate combustion. (3) Stabilization and propagation of flame in the combustion chamber.3.3.1 Heating valueIn most combustion problems any water produced by the reaction will be in the vapor state. If the latent heat of water is not included, the calorific value is referred to as the lower calorific value (LCV) H u. The relationship between higher(HCV) H u and lower calorific value is on gravimetric basis: H0-H u=wr. Where w is the mass of water per unit quantity of fuel and r is the enthalpy of evaporation of water at the temperature under consideration.3.3.2 Theoretical air of complete combustion of the fuelThe minimum amount of air that supplies sufficient oxygen for the complete combustion of all the carbon, hydrogen, and any other elements in the fuel that may oxidizes is called the “theoretical air”. When complete combustion is achieved with theoretical air, the products contain no oxygen.The average mass fraction of gasoline(kg): g c =0.855; g H =0.145;g O =0.000. The average mass fraction of diesel fuel(kg): g c =0.870; g H =0.126; g O =0.004. The needed oxygen mass(kg) for complete combustion of 1 kg fuel is:2.667g C +8g H -g O (kg)The “theoretical air ” L 0(kg) for complete combustion of 1 kg fuel can be calculated as:)8667.2(23.010o H c g g g L -+= For gasoline: L 0=14.9 (kg/kg). For diesel fuel : L 0=14.5 (kg/kg).3.3.3 Combustion stoichiometryAir-fuel ratio (AFR) is the mass ratio of air to fuel present in an internal combustion engine. It is an important measure for anti-pollution and performance-tuning reasons.fuel air m m F A AFR ==/ If exactly enough air is provided to completely burn all of the fuel, the ratio is known as the stoichiometric mixture, often abbreviated to stoich. The “theoretical air ” we discussed above is actually the stoichiometric air fuel ratio of the fuel. Fuel-air ratio is also used in studies of internal combustion engine, and refers to the ratio of fuel to the air.airfuel m m AFR FAR ==1 The ratio of the actual fuel/air ratio to the stoichiometric ratio (or its inverse) is a more informative parameter for defining mixture composition. The fuel/air equivalence ratio φ,stoich actual FAR FAR =φ stoichactual AFR AFR ==φλ1 φ<1, λ>1, AFR> 14.9→lean mixture,φ=1, λ=1, AFR= 14.9→stoichiometric mixture,φ>1, λ<1, AFR< 14.9→rich mixture.。

《发动机原理》双语教案(chapter 6)

《发动机原理》双语教案(chapter 6)

Chapter 6 Engine Operating CharacteristicsKey: Engine load characteristics, speed characteristics, universal characteristics Difficult points: Analyze the tendency of speed characteristics and its application.Section 1 Engine performance parameters6.1 Engine performance parametersThe practical engine performance parameters of interest are power, torque and specific fuel consumption. The relative importance of these parameters varies over an engine’s operating speed and load range. The maximum or normal rated brake power and the quantities such as bmep derived from it define an engine’s fullpotential.The interrelationship between engine performance parameters is the basis of engine characteristics analysis and the explanation of the curves. The relations between main parametersand procedure variables are given below:mPJFkWyMlq5cU6ANXgYbx5mE9KER6HzJ9SipLeDOBJPzqMHzvYqBZ5qht4wA (1) Brake power:(2) Brake torque: (3) Brake specific fuel consumption: (4) Fuel consumption rate: Where k 1,k 2,k 3,k 4 is constant;ηv is volumetric efficiency; λ is relative air/fuel ratio; ηi is indicated efficiency; ηm is mechanical efficiency; n is engine rotary speed.Section 2 Engine load characteristicsRelation between the instantaneous value of main engine economic parameters and engine load, when engine speed is maintained constant, is known as engine load characteristics.i m e K b ηη⋅⋅=13i m v tq K T ηηλη⋅⋅⋅=2nK p i m v e ⋅⋅⋅⋅=ηηλη1nK P b B v e e ⋅⋅==λη4The curve representation is known as load characteristics curve.6.2.1 Load characteristics of SI engine1. DefinitionOpening the throttle valve by matching increased dynamometers brake load gradually to keep the engine speed in constant ,the variation relations between engine brake specific fuel consumption b e and fuel consumption rate B with brake power P e (brake mean effective pressure P me,brake torque T tq ) is termed as load characteristics of SI engine.When the opening of throttle valve, bothηi and ηm rise, thus the bsfc b e drops drastically. As in heavy duty when rich mixture needed, incomplete combustion causes the decreases of indicated efficiency, this makes the bsfc b e rise up.6.2.2 Load characteristics of CI engineMoving the injector pump rack to change the oil supply Δb by applying matched dynamometers brake load to keep the engine speed in constant ,the variation relations between engine brake specific fuel consumption be and fuel consumption rate B with brake power P e (brake mean effective pressure P me ,brake torque T tq) is referred as load characteristics of CI engine.When the control rack or rod moving to positive direction for fuel injection, both ηi and ηm rise at the beginning, thus the bsfc b e drops drastically. Then richer mixture results in the decrease of indicated efficiency, but the ηm, counter action of the two variables form a relative horizontal line of bsfc b e in heavy loadoperation.6.2.3 Comparison of SI engine load characteristics with CI engine1. Bsfc of SI engine is higher than that of CI engineThe compression ratio of CI engine is more higher than that of SI engine, and the volumetric efficiency is higher too. SI engine burn with leaner mixture, that is to say, with excessive air, thus the indicated efficiency of CI engine is higher than that of SI engine, which results in the lower bsfc in CI engine.2. The curve of SI engine bsfc is more curvature than that of CI engine3. The exhaust temperature of SI engine is higher than that of CI engineThe higher compression ratio of CI engine gives a fully expansion of burnt charge, which results in the lower exhaust temperature more in SI engine.Section 3 Engine speed characteristicsWith the fuel control mechanism(rack,rod or throttle valve) fixed, the variation relations between engine main performance parameters(brake torque, brake power and bsfc) with engine speed is referred to engine speedcharacteristics.The characteristic derived with the fuel control mechanism fixed in maximum fuel supply position is termed as full-loadcharacteristics.6.3.1 Speed characteristics of SI engine1. DefinitionWith the throttle valve fixed, the variation relations between engine main performance parameters such as brake torque, brake power and bsfc with engine speed is referred to speed characteristics of SIengine.O6zM47DbzGfFj0Cg21SU8A61am2WoQWyYh7kW4U1eSAXci0rgzSvUjEeZyBI 1) Curve of brake torqueThe main factors that influence brake torque are ηi , ηm , ηv and λ.(1) Indicated efficiencyηi peaks at a middle speed ( Fig.7.6(a) ). While in too high engine speeds, the combustion duration counted with crank angle is extended, this reduces the combustible efficiency, thus the ηi.(2) Mechanical efficiencyηm decreases with increasing of engine speed ( Fig.7.6(b) ).When engine speeds up, increases in mechanical loss, accessories consumption and pumping loss decrease the mechanical efficiency. (3) V olumetric efficiencyηv peaks at certain engine speed ( Fig.7.6(c) ). With fixed throttle position and fixed valve timing, the volumetric efficiency curve rises slightly in low engine speed im v tq K T ηηλη⋅⋅⋅=2and drops drastically in high engine speed due to the fast growing frictional loss in inlet pipes and passages.(4) Relative A/F equivalence ratioλincreases modestly with increasing of engine speed ( Fig.7.6(d) ).It has modest effect on brake torque.2) Curve of brake powerWith increasing engine speed, the brake torque increases, so the brake power rises rapidly. As MBT is reached, the brake torque drops, which slow down brake power, and eventually turn it down when peak power is obtained.3) Curve of bsfcIn low engine speed range, ηi increase while ηm decrease with increasing engine speed, be decrease moderately. While in high engine speed range, bothηi and ηm decrease with increasing engine speed, thus be increases rapidly.6.3.2 Speed characteristics of CI engines1. DefinitionWith the fuel control mechanism(rack or rod) fixed, the variation relations between engine main performance parameters such as brake torque, brake power and bsfc with engine speed is referred to speed characteristics of CI engine.1) Curve of brake torqueIn diesel engine, the torque produced under certain engine speed is mainlyηVρhdetermined by circle fuel injection Δb . Heat addition per-cycle Δb is:So the cycle fuel injection Δb is: and the Ttq can be turned into: From the above equation, we can get that the main factors that influence brake torque are ηi , ηm and Δb.(1) Indicated efficiencyηi peaks at a middle speed(Fig.7.8).In the low engine speed range,the loss due to heat transfer is large,so ηi is low.While in high engine speeds range,reduced volumetric efficiency and increased Δb form richer mixture,resulting in the drop of indicated efficiency.(2) Mechanical efficiencyηm decreases with increasing engine speed ( Fig.7.8 ).When engine speeds up,increases in mechanical loss,accessoriesconsumption and pumping loss decrease the mechanical efficiency. (3) Fuel injection per-cycleΔb increases with increasing engine speed due to the throttle effect in injector pumps.2) Curve of brake powerWith increasing engine speed, the brake torque increases, so the brake power rises rapidly. As MBT is reached, the brake torque drops, which slow down the increase of brake power.3) Curve of bsfc00L V b s v λρη=∆b K T mi tq ∆=ηη2'In low engine speed range, ηi increase while ηm decrease with increasing engine speed, be decrease moderately. While in high engine speed range, bothηi and ηm decrease with increasing engine speed, thus be increases rapidly.6.3.3 Comparison of SI engine speed characteristics with CI engineDifferences between the two are the followings:(1)The torque curves of SI engine under all load range is relatively flat, while that of a SI engine drops drastically in high engine speed range.(2)The peak power can be reached in SI engine full-load power curve, ordinarily it is the rated power, while the peak point can hardly be reached in CI engine power curve.(3) The bsfc curves of CI engine under all load range is relatively flat, while that ofa SI engine is more warping, especially in low-load range.Section 4 Diesel engine governing characteristicsA device for automatically controlling the speed of an engine by regulating the intake or injection of fuel, so that the engine speed is maintained at the desired level under all conditions of loading, is termed the governor.With injector speed-regulating handle fixed and governor functioning, the variation relations of main performance parameters P e, T tq and b e of diesel engine withengine speed is referred to as governing characteristics.Two styles are used to illustrate governing characteristic:(1) load characteristic style(2) speed characteristic styleEngine speed governors can be classed as speed-limiting, constant-speed or all-speed type by function; or classified as mechanical, electronics, pneumatic and hydraulic type by structure.(1) Construction machinery and tractors are normlly equipped with constant-speed governor.(2)Automobile used engines are usually fitted with speed-limiting governors.Chapter 5 Engine universal characteristics One common way to present the operating characteristics of an engine over its full load and speed range is to plot brake specific fuel consumption contours on a graph of brake mean effective pressure versus engine speed.Maxmum bmep occurs in the mid-speed range; the minimum bsfc island is located at a slightly lower speed and at part load. These map characteristics can be understood in terms of variations in ηi ,ηm , ηv and the importance of heat losses and friction change.Engine performance map can be plotted by two methods: by speed characteristics or load characteristics.Comparison of universal characteristicsFirstly, bsfc be of SI engine is higher than that of CI engine;Secondly, the most economic region of SI engine located at the location of the upper, that is to say, high load areas. With the decrease of load, bsfc increases rapidly. As for CI engine, the most economic regions are more modest. When change load, the economic characteristic changes small.Because vehicle gasoline engine usually run at lower load, bsfc is high, economic characteristic is not good.For vehicle diesel engine, because more condition are used in truck, engineering machinery, mining vehicles, loads are high, the economic characteristic are better from universal characteristics curves.On the universal characteristic figure, specific fuel consumption curve at the innermost is equal to the most economic area that engine is running, the outward the contour curve, the worse economic characteristics.Shape and location of equivalence bsfc curve have important influence on actual economic characteristic.If the shape of curve is longer at horizontal direction, it shows that bsfc changes little when engine runs at loan changes little and speed changes great.If the shape of curve is longer at vertical direction, it shows that bsfc changes little when engine runs at loan changes great and speed changes little.For cars with internal combustion engine, the most economic region should beroughly in the intermediate position of the universal characteristics, so common speed and load can fall in the economic area, and specific fuel consumption curves in the transverse is longer than the other.For tractor and engineering machinery with internal combustion engine, the speed range is smaller and the load range is larger, the most economic region should be near the calibration speed, and a longer along the longitudinal.。

《发动机原理》(教案大纲)

《发动机原理》(教案大纲)

《发动机原理》教学大纲课程编码:课程名称:发动机原理英文名称:Fundamental of Automobile Engine开课学期:6学时/学分:64/4或36/2 (其中实验学时:8或4 )课程类型:专业课开课专业:热能与动力工程专业或车辆工程选用教材:《发动机原理》(第2版)林学东编著机械工业出版社2015.01执笔人:一、课程性质、目的与任务本课程是汽车发动机及车辆工程专业本科生必修的一门主要专业理论课。

本课程的目的是通过本课程的学习,使学生掌握发动机的能量转换的基本原理及其性能评价方法、影响发动机性能因素的分析方法;了解提高或改进发动机性能的主要途径和措施。

为合理使用、正确调整以及汽车动力传动系统合理匹限奠定理论基础;同时初步掌握发动机的试验方法和实验技能。

二、教学基本要求本课程主要讲述汽车发动机的工作原理及其特性,它以发动机性能指标为主要研究对象,介绍发动机的基本工作原理,分析影响内燃机各工作过程以及性能指标的各种因素。

从节能减排角度合理组织发动机工作过程以及如何提高其性能是本课程的中心内容。

通过本课程的学习,使学生牢固掌握发动机的性能指标、性能特性及其分析方法和主要影响因素;初步掌握发动机的试验方法及其数据处理和万有特性制取方法;为汽车动力系统合理匹时奠定理论基础。

根据总学时的要求,内容可根据具体培养要求进行删减。

三、各章节内容及学时分配第一章绪论教学目的与要求本章节着重介绍汽车发动机在国民经济中的重要作用。

通过本章的学习,使学生了解内燃机的发明与发展历程,以及不同阶段汽车发动机发明发展过程中存在的问题,正确对待发动机原理这门课程,正确对待以发动机为动力源的汽车发展对社会环境与文明的影响,明确本课程的学习目的和方法,培养对本课程的学习兴趣。

1.1本课程的任务、要求和学习方法1.2内燃机与汽车及其发展史简介1.3汽车工业的发展阶段1.4汽车发展对社会环境的影响考核要求:了解内燃机在国民经济中的作用、内燃机的发展历史、现状及趋势。

《发动机原理》双语教案(chapter 1)·优选.

《发动机原理》双语教案(chapter 1)·优选.

Chapter 1 Engine Thermodynamics and PerformanceParametersKey points: Concept of engine ideal cycle and real cycle; evaluation parameters of real cycle and purposes; mechanical losses and influent facts; engine heat energy balance.Difficult points: Evaluation indicators of engine dynamics and economics performance; the ways enhancing mechanical efficiency.1.1 Ideal air standard cycles1.1.1Simplified conditions for air standard cycle1)Assume that working medium is an ideal gas, and its physical constants are the same as air physical constants in standard condition.2)Assume that working medium is a closed loop in the closed system.3)Assume that the compression and expansion process is adiabatic (no heat transfer) and reversible, and thus isentropic process.4)Assume that combustion is addition of heat Q1 at constant volume or pressure from innumerable high temperature heat source. Rejection of heat Q2 at constant volume to complete the cycle.1.1.2 Three basic cyclesOtto cycle:Ideal cycle of gasoline engine.Diesel cycle:Ideal cycle of large low-speed diesel.Mixed cycle:Ideal cycle of high-speed diesel.1.1.3 The parameters assessing the theoretical circle are cycle fuel conversion efficiency ηt and mean effective pressure p t.1.1.4 Cycle fuel conversion efficiency ηtThe cycle fuel conversion efficiency ηt is used to evaluate the cycle economy, which is defined as:1212111Q Q Q Q Q Q W t -=-==η (1.1)Where W=work output; Q 1=cycle heat addition; Q 2=cycle heat rejection.The cycle thermal efficiency of standard dual cycle can be derived by thermodynamic equation:()()111111-+--⋅-=-ρλλληρεK KK tm (1.2) Where ε=compression ratio, ε=V a /V c =(V s +V c )/V c =1+V s /V c , in which V a =cylinder displacement, V c =combustion chamber clearance, V s =swept volume; λ=pressure ratio during constant -volume heat addition, λ=p z /p c ;ρ= volumetric expansion ratio during constant-pressure heat addition , ρ=V z /V z ’; K= isentropic exponent.We can draw a conclusion by eq.(1.2) that t η increases with the increasing of compression ratio ε, pressure ratio λ, isentropic exponent K and de creases with the increasing of expansion ratio ρ.1.1.5 Mean effective pressureMean effective pressure p t (MPa) is cycle work done by unit cylinder volume. It is used to evaluate the power capability of a cylinder and is defined as follow:s t V Wp = (1.3)Where W (kJ )= cycle work done by the cylinder; V s (L) = swept volume.We can also deduce the mean effective pressure of dual cycle by thermodynamic equation:t a Ktm K K p p ηρλλεε⋅-+-⋅-⋅-=)]1()1[(11 (1.4) Where p a = cylinder pressure when inlet valve is closed.From Eq.(1.4) ,a conclusion can be drawn that pt increases with increasing of pressure p a , compression ratio ε, pressure ratio λ, expansion ratio ρ, isentropic exponent K and cycle thermal efficiency t η.1.2Real cycles of Four-Strokes Engine1.2.1 Real cycle p-V diagram of four-stroke engineReal cycles: engine real cycles is composed of induce, compress, combustion, expansion and exhaust five processes. They are more complicate than ideal cycles. Usually they can be indicated by p-V diagram which represents pressure in cylinder changes with work volume of cylinder.1.Intake strokeDuring this stroke, the piston is moving downward and the intake valve is open. This downward movement produces a partial vacuum in the cylinder, and air and duel rush into the cylinder past the open intake valve.pression strokeThe intake valve closes and seals the upper end of the cylinder. As the crankshaft continues to rotate, it pushes the connecting rod up against the piston. The piston then moves upward and compresses the combustible mixture in the cylinder. Compressing the mixture in this way makes it more combustible; not only does the pressure in the cylinder go up, but the temperature of the mixture also increases.3.Power strokeAs the piston reaches top dead center at the end of the compression stroke, the ignition system produces an electric spark. The spark sets fire to the fuel-air mixture. In burning, the mixture gets very hot and expands in all directions. The pressure rises to about 600 to 700 pounds per square inch. Since the piston is the only part that can move, the force produced by the expanding gases forces the piston down. This force is given a power twist.4.Exhaust strokeThe exhaust valve opens as the power stroke is finished and the piston starts back up on the exhaust stroke.1.2.2 Comparison with ideal cyclesThe expansion stroke pressures for the engine fall below the fuel-air cycle pressures for the following reasons:(1) heat transfer from the burned gases to the walls;(2) finite time required to burn the charge;(3) incomplete combustion of the charge;(4) exhaust blowdown loss due to opening the exhast valve beforE BDC;(5) gas flow into crevice regions and leakage past the piston rings;(6)pumping loss.1.3 Indicated engine performance parametersThe parameters which are calculated on basis of the work done by working fluid to pistons are called indicated parameters. It is widely used to evaluate the conversion efficiency of heat into power per cycle and is widely used in engine research field. 1、Indicated work per cycle W iPressure data for the gas in the cylinder over the operating cycle of the engine can be used to calculate the work transfer from the gas to the piston.The indicated work per cycle W i (per cylinder) is obtained by integrating around the curve to obtain the area F i enclosed on the diagram.W i = F i ΔWhere W i (kJ) = the net indicated work per cycle;F i (cm 2) = net area wrapped in the diagram;Δ(kJ/cm 2)= the plotting scale, 1cm 2 area in the diagram represents Δ kJ work.2. Indicated mean effective pressure (imep) p miThe imep is a measure of the indicated work output per unit swept volume, in a form independent of the size and number of cylinders in the engine and engine speed. )()/()/(32m V m N W m N imep p s i mi == Where W i = indicated work per cylinder per cycle;V s = swept volume per cylinder.Figure shows an indicator diagram with a shaded area, equal to the net area ofthe indicated diagram. In a four-stroke cycle the negative work occurring during the induction and exhaust strokes is termed pumping loss, and has to be subtracted fromthe positive indicated work of the other two strokes.gross imep = net imep + pmep.3. Indicated power P iIndicated work done by an engine in unit time is referred to as indicated power P i .Suppose that an engine has a number of cylinders i, the diameter of cylinders is D(m), swept volume is V s (m 3), imep is p m (N/m 2), engine rotary speed is n (r/s). In practical application, p mi (MPa), V(L), n (r/min) are adopted, so the indicated power can be calculated as followτ30)ni V p kW P s mi i =( (1.5) 32104-⨯==S D p V p W mi s mi i π ττ30260in V p i n W P s i m i i ==Where τ= 2 for 2-stroke engine and τ= 4 for 4-stroke engine.4. Indicated efficiency ηiWhen comparing the performance of engines it is sometimes useful to isolate the mechanical losses. This leads to the use of indicated (arbitrary overall) efficiency as a means of examining the thermodynamic processes in an engine:1Q W ii =ηWhere Q 1 = heat addition per cylinder per cycle.Indicated efficiency ηi is a dimensionless parameter, it has another expression:ui i BH P 3106.3⨯=η (1.6) In which, B(kg/h) = the mass of fuel inducted per hour,H u (kJ/kg) = low calorific value of the fuel.5. Indicated specific fuel consumption b iIndicated specific fuel consumption (isfc ) is the fuel flow rate per unit power output on basis of working fluid to pistons. If the mass of fuel inducted per hour B and indicated power P i are given, then:310)()/()/((⨯=⋅kW P h kg B h kW g b i i (1.7)The relationship between ηi and b i can be given by incorporating Eq. 1.6 and Eq. 1.7:iu i b H 6106.3⨯=η1.4 Engine brake performance parametersEngine brake parameters are parameters based on engine crankshaft output work. It is used to evaluate economic and dynamic performance of an engine.1. Brake torque T tq and power P eEngine torque T tq is normally measured with a dynamometer: T tq = Fb.The power P e delivered by the engine and absorbed by the dynamometer is the product of torque and angular speed: P e = 2πnT tq .9550min)/()()(r n m N T kW P tq e ⋅=2. Brake work W e and brake mean effective pressure p meThe work output of an engine is brake work, as measured by a brake or dynamometer. The difference between indicated work and brake work is accounted for by friction, and work done in driving essential items such as the lubricating oil pump. W e = W i -W m , where W m = work of mechanical loss.Brake mean effective pressure (bmep) is based on the work available as output from the engine:)()/()/(32m V m N W m N bmep p s e me == Similar to Eq. 1.6, we have: τ30)(ni V p kW P s me e =3. Brake(thermal) efficiency ηe The ratio of the work produced per cycle to the amount of fuel energy supplied per cycle that can be released in the combustion process is commonly used for this purpose. It is a measure of the engine ’s efficiency.1Q W ee =ηWhere Q 1=heat addition per cylinder per cycle.It can be calculated by another way: ue e BH P 3106.3⨯=η 4. Brake specific fuel consumption (bsfc) b e :Brake specific fuel consumption (bsfc) is the fuel flow rate per unit power output on basis of engine flywheel engine.1000⨯=e e P B bThe relationship between ηe and b e is:6106.3⨯=μηh b e e5. Engine specific weight m e and specific volume V eThree parameters useful for comparing these attributes from one engine toanother are: e e P m m =where m= weight of engine, P e is rated power.es e P iV V =where iV s = bulk volume of engine. ττ3030n p i V in V p i V P P mes s me s e L ===1.5 Engine mechanical efficiency and energy balance1.5.1 Mechanical efficiencyAll these make differences between indicated and brake power and can be given in detail as following:Pumping power, defined as the net work per unit time done by the piston on the gases during the inlet and exhaust strokes.Compressor power, that is, power taken from the crankshaft to drive ascavenging pump or supercharger.Auxiliary power, the power required to drive auxiliaries, such as oil pump, water pump, cooling fan, and generator.Friction power, the power used to overcome the friction of the bearings, pistons and so on.Turbine power. In some engines an exhaust turbine has been geared to thecrankshaft. In such cases the power developed by the turbine will add to the brake power of the engine and could be classed as a “negative ” friction loss.All the “loss ” above can be evaluated by mechanical loss power P m as well as p mm -mechanical mean effective pressure(mmep), the part of the indicated mean effective pressure used to overcome mechanical friction.inV P p s m mm τ30= The ratio of the brake(or useful) power delivered by the engine to the indicated power is called the mechanical efficiency ηm :i m i e m P P P P -==1η It can also be defined as:mimm mi me i e m p p P P W W -===1η1.5.2 Engine energy balance1. Heat discharged by fuel combustion Q T (kJ/h): Q T =BH u2. Heat converted to brake work Q E (kJ/h): Q E =3.6×103P e3. Heat transferred to cooling medium Q S (kJ/h):Q s =G s c s (t 2-t 1)4. Heat transferred to exhaust system Q R (kJ/h):Q R =(B+G K )(c pr t 2-c pk t 1)5. Energy loss due to incomplete combustion Q B :Q B =Q T (1-ηr )6. Other energy losses Q L : All other energy losses not discussed above are covered by Q L .An energy balancing equation can be described as:Q T =Q E +Q S +Q R +Q B +Q L最新文件---------------- 仅供参考--------------------已改成word 文本 --------------------- 方便更改。

发动机原理初中生物教案

发动机原理初中生物教案

发动机原理初中生物教案
目标:通过本节课的学习,学生能够理解发动机的工作原理以及其在日常生活中的应用。

教学目标:
1. 了解发动机是什么,以及它的作用;
2. 掌握发动机的工作原理;
3. 能够简单描述发动机如何在汽车等交通工具中发挥作用。

教学内容:
1. 什么是发动机;
2. 发动机的工作原理;
3. 发动机在日常生活中的应用。

教学准备:
1. 图片或视频展示发动机的外观和结构;
2. 模型或示意图来演示发动机的工作原理;
3. 笔记本和笔。

教学过程:
1. 引入:用图片或视频展示发动机的外观和结构,让学生猜测发动机是用来做什么的。

2. 发展:简要介绍发动机是用来产生动力的机器,它可以将燃料转化为能量,驱动交通工具运行。

3. 发动机的工作原理:通过模型或示意图演示发动机的工作原理,包括燃烧室、活塞、曲轴等组成部分在工作时的运动和作用。

4. 应用举例:结合汽车、飞机等交通工具,让学生理解发动机在这些机器中的作用和重要性,以及如何通过改变发动机的设计来提高性能。

5. 练习:让学生回答一些与发动机相关的问题,加深他们对课程内容的理解。

6. 总结:对本节课学习的内容进行总结,强调发动机在日常生活中的应用和重要性。

教学反思:
这节课的主要目标是让学生了解发动机的定义和工作原理,以及发动机在日常生活中的应用。

通过图像、模型和示意图等多样化的教学手段,可以帮助学生更好地理解和记忆发动
机的工作原理,同时也能够提高他们的学习兴趣和参与度。

在教学中要注重与学生的互动,引导他们主动思考问题,培养他们的创造力和实践能力。

发动机原理初中生物教案

发动机原理初中生物教案

发动机原理初中生物教案课程目标:1. 了解发动机的基本组成和工作原理。

2. 掌握发动机的四个冲程及其作用。

3. 理解发动机的效率和性能指标。

教学重点:1. 发动机的基本组成。

2. 发动机的工作原理和四个冲程。

教学难点:1. 发动机的效率和性能指标。

教学准备:1. 发动机模型或图片。

2. 发动机工作原理图。

教学过程:一、导入(5分钟)1. 引入话题:介绍发动机在日常生活中的应用,如汽车、摩托车等。

2. 提问:同学们知道发动机是什么吗?它有什么作用?二、讲解发动机的基本组成(10分钟)1. 介绍发动机的各个部分,包括气缸、活塞、曲轴、进气门、排气门等。

2. 讲解各部分的作用和相互之间的关系。

三、讲解发动机的工作原理(10分钟)1. 介绍发动机的工作原理,包括四个冲程:进气冲程、压缩冲程、做功冲程、排气冲程。

2. 讲解每个冲程的作用和特点。

四、讲解发动机的效率和性能指标(10分钟)1. 介绍发动机的效率,包括热效率和机械效率。

2. 讲解发动机的性能指标,如功率、扭矩、燃油消耗率等。

五、实践操作(15分钟)1. 观察发动机模型或图片,让学生更直观地了解发动机的各个部分。

2. 引导学生分析发动机工作原理图,理解四个冲程的作用和相互之间的关系。

六、总结和布置作业(5分钟)1. 总结本节课的主要内容,让学生巩固所学知识。

2. 布置作业:让学生绘制发动机工作原理图,并写一篇关于发动机原理的小论文。

教学反思:通过本节课的教学,学生应该能够了解发动机的基本组成、工作原理和性能指标。

在教学过程中,要注意引导学生积极参与,提问和解答问题,以提高学生的学习兴趣和动力。

同时,通过实践操作和绘制原理图,让学生更直观地理解发动机的工作原理,提高学生的动手能力和思维能力。

汽车专业英语 教案Unit 5Principle and Structure of Engine

汽车专业英语 教案Unit 5Principle and Structure of Engine

Translation Difficulties
1.Most automobile engines are internal combustion, reciprocating 4-stroke gasoline engines, but other types have been used, including the diesel, the rotary (Wankel), the 2-stroke, and stratified charge. 翻译:大多数汽车的发动机是内燃机,往复四冲程汽油机,但是也有使用其它类型的发动机, 包括柴油机,转子发动机,二冲程发动机和分程燃烧发动机。
[ˈkræŋkʃæft] [kəmˈprɛʃən] [ɪɡˈzɔst]
tightly
lubrication definite frame
[ˈtaɪtlɪ]
[ˌlubrɪˈkeʃən] [ˈdɛfənɪt] [frem]
bottom
[ˈbɑ:təm]
nickle chromium chamber
['nɪkəl] [ˈkroʊmiəm] [ˈtʃembɚ]
[sərˈkʌmfərəns]
n.曲柄针,曲柄梢 adj.孤僻的,离群的;偏僻的 v.取回,收回( withdraw 的过去分词) n.比,比率;[数学]比例(法);面积;相称,平衡 vt.使成比例;使相称;使均衡 复数:proportions n.周围,圆周;胸围 复数:circumferences
日期: 年 月 日
汽车英语教案
课题: Unit 5: Principle and Structure of Engine
目的要求:1.了解发动机的基本结构和组成; 2.掌握发动机的工作原理。

《发动机原理》双语教案(chapter 1)

《发动机原理》双语教案(chapter 1)

Chapter 1 Engine Thermodynamics and PerformanceParametersKey points: Concept of engine ideal cycle and real cycle; evaluation parameters of real cycle and purposes; mechanical losses and influent facts; engine heat energy balance.Difficult points: Evaluation indicators of engine dynamics and economics performance; the ways enhancing mechanical efficiency.1.1 Ideal air standard cycles1.1.1Simplified conditions for air standard cycle1)Assume that working medium is an ideal gas, and its physical constants are the same as air physical constants in standard condition.2)Assume that working medium is a closed loop in the closed system.3)Assume that the compression and expansion process is adiabatic (no heat transfer) and reversible, and thus isentropic process.4)Assume that combustion is addition of heat Q1 at constant volume or pressure from innumerable high temperature heat source. Rejection of heat Q2 at constant volume to complete the cycle.1.1.2 Three basic cyclesOtto cycle:Ideal cycle of gasoline engine.Diesel cycle:Ideal cycle of large low-speed diesel.Mixed cycle:Ideal cycle of high-speed diesel.1.1.3 The parameters assessing the theoretical circle are cycle fuel conversion efficiency ηt and mean effective pressure p t.1.1.4 Cycle fuel conversion efficiency ηtThe cycle fuel conversion efficiency ηt is used to evaluate the cycle economy, which is defined as:1212111Q Q Q Q Q Q W t -=-==η (1.1)Where W=work output; Q 1=cycle heat addition; Q 2=cycle heat rejection.The cycle thermal efficiency of standard dual cycle can be derived by thermodynamic equation:()()11111-+--⋅-=ρλλληρεK Ktm (1.2) Where ε=compression ratio, ε=V a /V c =(V s +V c )/V c =1+V s /V c , in which V a =cylinder displacement, V c =combustion chamber clearance, V s =swept volume; λ=pressure ratio during constant-volume heat addition, λ=p z /p c ;ρ= volumetric expansion ratio during constant-pressure heat addition , ρ=V z /V z ’; K= isentropic exponent.We can draw a conclusion by eq.(1.2) that t η increases with the increasing of compression ratio ε, pressur e ratio λ, isentropic exponent K and decreases with the increasing of expansion ratio ρ.1.1.5 Mean effective pressureMean effective pressure p t (MPa) is cycle work done by unit cylinder volume. It is used to evaluate the power capability of a cylinder and is defined as follow:s t V Wp = (1.3)Where W (kJ )= cycle work done by the cylinder; V s (L) = swept volume.We can also deduce the mean effective pressure of dual cycle by thermodynamic equation:t a Ktm K K p p ηρλλεε⋅-+-⋅-⋅-=)]1()1[(11 (1.4) Where p a = cylinder pressure when inlet valve is closed.From Eq.(1.4) ,a conclusion can be drawn that pt increases with increasing of pressure p a , compression ratio ε, pressure ratio λ, expansion ratio ρ, isentropic exponent K and cycle thermal efficiency t η.1.2Real cycles of Four-Strokes Engine1.2.1 Real cycle p-V diagram of four-stroke engineReal cycles: engine real cycles is composed of induce, compress, combustion, expansion and exhaust five processes. They are more complicate than ideal cycles. Usually they can be indicated by p-V diagram which represents pressure in cylinder changes with work volume of cylinder.1.Intake strokeDuring this stroke, the piston is moving downward and the intake valve is open. This downward movement produces a partial vacuum in the cylinder, and air and duel rush into the cylinder past the open intake valve.pression strokeThe intake valve closes and seals the upper end of the cylinder. As the crankshaft continues to rotate, it pushes the connecting rod up against the piston. The piston then moves upward and compresses the combustible mixture in the cylinder. Compressing the mixture in this way makes it more combustible; not only does the pressure in the cylinder go up, but the temperature of the mixture also increases.3.Power strokeAs the piston reaches top dead center at the end of the compression stroke, the ignition system produces an electric spark. The spark sets fire to the fuel-air mixture. In burning, the mixture gets very hot and expands in all directions. The pressure rises to about 600 to 700 pounds per square inch. Since the piston is the only part that can move, the force produced by the expanding gases forces the piston down. This force is given a power twist.4.Exhaust strokeThe exhaust valve opens as the power stroke is finished and the piston starts back up on the exhaust stroke.1.2.2 Comparison with ideal cyclesThe expansion stroke pressures for the engine fall below the fuel-air cycle pressures for the following reasons:(1) heat transfer from the burned gases to the walls;(2) finite time required to burn the charge;(3) incomplete combustion of the charge;(4) exhaust blowdown loss due to opening the exhast valve beforE BDC;(5) gas flow into crevice regions and leakage past the piston rings;(6)pumping loss.1.3 Indicated engine performance parametersThe parameters which are calculated on basis of the work done by working fluid to pistons are called indicated parameters. It is widely used to evaluate the conversion efficiency of heat into power per cycle and is widely used in engine research field. 1、Indicated work per cycle W iPressure data for the gas in the cylinder over the operating cycle of the engine can be used to calculate the work transfer from the gas to the piston.The indicated work per cycle W i (per cylinder) is obtained by integrating around the curve to obtain the area F i enclosed on the diagram.W i = F i ΔWhere W i (kJ) = the net indicated work per cycle;F i (cm 2) = net area wrapped in the diagram;Δ(kJ/cm 2)= the plotting scale, 1cm 2 area in the diagram represents Δ kJ work.2. Indicated mean effective pressure (imep) p miThe imep is a measure of the indicated work output per unit swept volume, in a form independent of the size and number of cylinders in the engine and engine speed.)()/()/(32m V m N W m N imep p s i mi == Where W i = indicated work per cylinder per cycle;V s = swept volume per cylinder.Figure shows an indicator diagram with a shaded area, equal to the net area of the indicated diagram. In a four-stroke cycle the negative work occurring during the induction and exhaust strokes is termed pumping loss, and has to be subtracted fromthe positive indicated work of the other two strokes.gross imep = net imep + pmep.3. Indicated power P iIndicated work done by an engine in unit time is referred to as indicated power P i .Suppose that an engine has a number of cylinders i, the diameter of cylinders is D(m), swept volume is V s (m 3), imep is p m (N/m 2), engine rotary speed is n (r/s). In practical application, p mi (MPa), V(L), n (r/min) are adopted, so the indicated power can be calculated as followτ30)ni V p kW P s mi i =( (1.5) 32104-⨯==S D p V p W mi s mi i π ττ30260in V p i n W P s i m i i == Where τ= 2 for 2-stroke engine and τ= 4 for 4-stroke engine.4. Indicated efficiency ηiWhen comparing the performance of engines it is sometimes useful to isolate the mechanical losses. This leads to the use of indicated (arbitrary overall) efficiency as a means of examining the thermodynamic processes in an engine:1Q W ii =ηWhere Q 1 = heat addition per cylinder per cycle.Indicated efficiency ηi is a dimensionless parameter, it has another expression:ui i BH P 3106.3⨯=η (1.6) In which, B(kg/h) = the mass of fuel inducted per hour,H u (kJ/kg) = low calorific value of the fuel.5. Indicated specific fuel consumption b iIndicated specific fuel consumption (isfc ) is the fuel flow rate per unit power output on basis of working fluid to pistons. If the mass of fuel inducted per hour B and indicated power P i are given, then:310)()/()/((⨯=⋅kW P h kg B h kW g b i i (1.7)The relationship between ηi and b i can be given by incorporating Eq. 1.6 and Eq. 1.7:iu i b H 6106.3⨯=η1.4 Engine brake performance parametersEngine brake parameters are parameters based on engine crankshaft output work. It is used to evaluate economic and dynamic performance of an engine.1. Brake torque T tq and power P eEngine torque T tq is normally measured with a dynamometer: T tq = Fb.The power P e delivered by the engine and absorbed by the dynamometer is the product of torque and angular speed: P e = 2πnT tq .9550min)/()()(r n m N T kW P tq e ⋅=2. Brake work W e and brake mean effective pressure p meThe work output of an engine is brake work, as measured by a brake or dynamometer. The difference between indicated work and brake work is accounted for by friction, and work done in driving essential items such as the lubricating oil pump. W e = W i -W m , where W m = work of mechanical loss.Brake mean effective pressure (bmep) is based on the work available as output from the engine:)()/()/(32m V m N W m N bmep p s e me == Similar to Eq. 1.6, we have: τ30)(ni V p kW P s me e =3. Brake(thermal) efficiency ηe The ratio of the work produced per cycle to the amount of fuel energy supplied per cycle that can be released in the combustion process is commonly used for this purpose. It is a measure of the engine ’s efficiency.1Q W ee =ηWhere Q 1=heat addition per cylinder per cycle.It can be calculated by another way: ue e BH P 3106.3⨯=η 4. Brake specific fuel consumption (bsfc) b e :Brake specific fuel consumption (bsfc) is the fuel flow rate per unit power output on basis of engine flywheel engine.1000⨯=e e P B bThe relationship between η e and b e is:6106.3⨯=μηh b e e5. Engine specific weight m e and specific volume V eThree parameters useful for comparing these attributes from one engine to another are:ee P m m = where m= weight of engine, P e is rated power.es e P iV V =where iV s = bulk volume of engine. ττ3030n p i V in V p i V P P mes s me s e L ===1.5 Engine mechanical efficiency and energy balance1.5.1 Mechanical efficiencyAll these make differences between indicated and brake power and can be given in detail as following:Pumping power, defined as the net work per unit time done by the piston on the gases during the inlet and exhaust strokes.Compressor power, that is, power taken from the crankshaft to drive a scavenging pump or supercharger.Auxiliary power, the power required to drive auxiliaries, such as oil pump, water pump, cooling fan, and generator.Friction power, the power used to overcome the friction of the bearings, pistons and so on.Turbine power. In some engines an exhaust turbine has been geared to the crankshaft. In such cases the power developed by the turbine will add to the brake power of the engine and could be classed as a “negative ” friction loss.All the “loss ” above can be evaluated by mechanical loss power P m as well as p mm -mechanical mean effective pressure(mmep), the part of the indicated mean effective pressure used to overcome mechanical friction.inV P p s m mm τ30= The ratio of the brake(or useful) power delivered by the engine to the indicated power is called the mechanical efficiency ηm :i m i e m P P P P -==1η It can also be defined as:mimm mi me i e m p p P P W W -===1η1.5.2 Engine energy balance1. Heat discharged by fuel combustion Q T (kJ/h): Q T =BH u2. Heat converted to brake work Q E (kJ/h): Q E =3.6×103P e3. Heat transferred to cooling medium Q S (kJ/h):Q s =G s c s (t 2-t 1)4. Heat transferred to exhaust system Q R (kJ/h):Q R =(B+G K )(c pr t 2-c pk t 1)5. Energy loss due to incomplete combustion Q B :Q B =Q T (1-ηr )6. Other energy losses Q L : All other energy losses not discussed above are covered by Q L .An energy balancing equation can be described as:Q T =Q E +Q S +Q R +Q B +Q L。

发动机原理教案范文

发动机原理教案范文

发动机原理教案范文标题:发动机原理教案教学目标:1.了解发动机的基本原理和工作过程;2.掌握不同类型发动机的特点和应用;3.培养学生对发动机技术的兴趣和实践能力;4.培养学生的创新思维和动手能力。

教学重点:1.原理:发动机的基本组成和工作原理;2.分类:内燃机和外燃机的区别及各自特点。

教学时长:2个课时教学内容及过程:第一课时一、导入(5分钟)1.教师引入话题:你有没有想过汽车是如何运转的?是什么让汽车产生动力?2.学生参与讨论,分享他们的想法和观点。

二、发动机的基本组成(15分钟)1.通过图片和实物展示,介绍发动机的基本组成部分:气缸、活塞、曲轴、气门、喷油器、燃油系统等。

2.引导学生仔细观察和讨论各个部件的功能和相互作用。

三、发动机的工作原理(25分钟)1.介绍发动机的工作原理:进气、压缩、燃烧和排气四个工作过程。

2.使用动画、实物或模型演示发动机的工作原理。

3.引导学生思考问题:为什么发动机需要进行压缩?燃烧后产生的能量如何转化为动力?四、内燃机与外燃机的区别(15分钟)1.介绍内燃机和外燃机的区别:内燃机燃料在燃烧室内直接燃烧,外燃机燃料在燃烧室外燃烧。

2.分析内燃机和外燃机的各自特点和应用领域。

五、小结(5分钟)总结本节课的内容,强调发动机的基本组成和工作原理。

第二课时一、复习(10分钟)1.让学生展示他们对上节课内容的理解:发动机的基本组成和工作原理。

2.教师进行必要的补充和点评。

二、不同类型的发动机(20分钟)1.介绍常见的发动机类型:汽油发动机、柴油发动机、氢燃料电池发动机等。

2.分析各种发动机的特点、优缺点和应用领域。

三、动手实践(30分钟)1.将学生分为小组,每个小组选择一种发动机进行深入研究。

2.学生根据指导和教师的辅导,动手拆装发动机模型,了解发动机内部结构和工作原理。

3.学生讨论并总结拆卸过程中的发现和心得。

四、发表成果(10分钟)1.每个小组展示他们拆装的发动机模型,介绍所选择的发动机类型和相关知识。

柴油机工作原理(双语教学)

柴油机工作原理(双语教学)

Now class begins.Today we shall study lesson 2: how does a diesel engine works.First let ’ review our last lesson;The first question what is the basic feature of marine diesel engine: from the last lesson we know marine diesel engine is a kind of internal combustion engine, and the fuel is ignited by compression, and the piston is reciprocating in the cylinder.The second question: Classification of marine diesel engine.We can classify diesel engine by its working cycle or structural feature.According to its working cycle, it is classified into 2 stroke and 4 stroke engine.What is stroke? For a cylinder, the distance from BDC to TDC is called a stroke. According to its structural feature, diesel engine is classified into trunk piston diesel and Crosshead diesel.Now let us begin our new lesson: the working principle of marine diesel engine. The main content is as follows:四冲程柴油机工作原理、二冲程柴油机工作原理、二冲程柴油机的换气形式。

发动机原理—教案

发动机原理—教案

【发动机原理】教案教材: 《汽车发动机原理》张志沛主编大连海运学院出版社长安大学汽车学院机电与动力研究所目录绪论------------------------------------------------------------------------------------------1第一章发动机工作循环及性能指标---------------------------------------------------------5§1-1发动机理想循环概述---------------------------------------------------------- 5§1-2发动机实际循环---------------------------------------------------------------7§1-3 热平衡------------------------------------------------------------------------8§1-4 指示指标-----------------------------------------------------------------------9§1-5 有效指标---------------------------------------------------------------------- 1 1§1-6 机械损失---------------------------------------------------------------------- 1 3§1-7 燃烧热化学-------------------------------------------------------------------- 1 6§1-8 发动机混合气的着火和燃烧方式----------------------------------------------- 20 第二章发动机的换气过程-------------------------------------------------------------------- 22§2-1 四冲程发动机的换气过程------------------------------------------------------ 2 2§2-2 四冲程发动机的充气效率------------------------------------------------------ 2 3§2-3 影响充气效率的各种因素------------------------------------------------------ 2 5§2-4 提高充气效率的措施---------------------------------------------------------- 27§2-5 进气管内的动态效应---------------------------------------------------------- 29§2-6 单位时间充气量与循环充气量------------------------------------------------- 30 第三章柴油机混合气形成和燃烧------------------------------------------------------------ 32§3-1 柴油机混合气形成------------------------------------------------------------ 3 2§3-2 柴油机的燃烧过程------------------------------------------------------------ 3 6§3-3 柴油机供油系统的工作特性及其对燃烧过程的影响---------------------------- 39§3-4 柴油机的燃烧室-------------------------------------------------------------- 41 第四章汽油机混合气形成和燃烧----------------------------------------------------------- 46§4-1 汽油机混合气形成------------------------------------------------------------ 4 6§4-2 汽油机的燃烧过程------------------------------------------------------------ 49§4-3 汽油机的燃烧室-------------------------------------------------------------- 57 第五章发动机噪声及排放污染-------------------------------------------------------------- 60§5-1 发动机噪声污染及防治------------------------------------------------------- 60§5-2 发动机排放污染及防治------------------------------------------------------- 63 第六章发动机特性--------------------------------------------------------------------------- 66§6-1 发动机工况和性能指标分析式------------------------------------------------ 66§6-2 发动机速度特性-------------------------------------------------------------- 66§6-3 发动机负荷特性-------------------------------------------------------------- 70§6-4 发动机万有特性-------------------------------------------------------------- 72§6-5 发动机调速特性-------------------------------------------------------------- 73§6-6 大气修正--------------------------------------------------------------------- 77 第七章发动机台架试验---------------------------------------------------------------------- 79§7-1 测量与计算参数-------------------------------------------------------------- 79§7-2 参数的测量------------------------------------------------------------------- 79§7-3 测取方法--------------------------------------------------------------------- 83第八章车用发动机的废气涡轮增压概述--------------------------------------------------- 85绪论能量转换:发动机-燃料的化学能→热能→机械能机械能、电能等-高级能源;热能-低级能源《发动机原理》课研究:热能→机械能(转换效率:理论上小于100%)机械能→热能(转换效率:理论上可达100%)发动机:内燃机和外燃机车用发动机:间歇工作式发动机四个冲程中只有一个冲程做功,做功不连续。

发动机原理课程教学大纲

发动机原理课程教学大纲

发动机原理》课程教学大纲一、课程性质与目的 Teaching Objective and Requirement 《发动机原理》是为汽车设计方向和汽车电子方向讲述车用发动机的基本 理论的专业课程, 是以内燃机原理为主要内容, 以内燃机的性能指标作为主要研 究对象, 明确各种因素对性能指标的影响规律及其相互之间的内在联系, 把合理 组织内燃机的工作过程, 提高整机性能作为中心内容。

同时还按专题介绍内燃机 工作过程中的一些特殊问题。

通过授课使学生初步掌握车用发动机的工作原理, 初步进行内燃机性能的评判、匹配和选用的能力。

《 Principle of Internal Combustion Engine 》 is a basic theory of professionalcourses which is set for the students whose major are automotive design and automotive electronics. The main content of this courses is the Principles and performance of the internal combustion engine. The main object is to clear the various factors on the performance and its mutual intrinsic link between each other, to improve the working process and its overall performance for engines. Presentations also some special problems in the process of internal combustion engines. Through lectures, students initially grasp the capacity of car engine works, preliminary performance evaluation of the internal combustion engine, matching and selection.二、课程基本要求 Basic requirement 熟悉内燃机工作过程的基本理论;熟悉内燃机的动力性、经济性和排放性 能指标;掌握汽油机、柴油机的混合气供给、混合气形成、燃烧过程;掌握内燃 机的运行特性及与动力机械的匹配; 了解内燃机的排放、 噪声、增压、代用燃料。

《发动机原理》双语教案(chapter4)

《发动机原理》双语教案(chapter4)

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 factorsSection 1 Introduction to spark ignition engine In 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 be divided into three parts: fuel delivery system, air induction system, and the electronic control system.1.Air induction systemWhen 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 runner to the intake valve.2.fuel delivery systemFuel 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 delivered to the intake manifold by the injector is returned to the tank through a fuel return pipe.3.electronic control systemThe 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 time , 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 Normal combustionWhen 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 ofsize as the turbulence scale, the flame propagation cannot be enhanced by the turbulence.1.Delay period—from A to B (first stage)This early burn period comprises the initial laminar combustion, and the transition to fully turbulent combustion, 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 to denote the end of the delay period.The delay period is typically of 1-2 ms duration, and this corresponds to 15-30°of 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 stoichiometric mixtures, in other words, when the laminar flame speed is highest.2. Second stage(fast combustion) ---from B to CThe 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 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 approximatelyconstant 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, we use λp 〔MPa /(º)〕to evaluate the pressure rise rate, and λp is normally between 0.20~0.40 MPa/(º)3. The final stage---after CThe 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, 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 propagation in enginesIn 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 sum 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: m L L F v dtdm ρ= Where m is the mass of mixture, v L is the propagation velocity of laminar flame front, F L is the superficial area of laminar flame front and ρm is density of end gas. The burning velocity of turbulent flame can be derived as: m T T F v dtdm ρ= Where m is the mass of mixture, v L is the propagation velocity of turbulent flame front, F L is the superficial area of turbulent flame front and ρm is density of end gas.There are several factors which affect the flame speed, including turbulence, fuel/air ratio, temperature and pressure, compression ratio, engine speed.4.2.3 Cyclic variation in combustion1. Cycle-by-cycle variations in combustionIt is also called cyclic dispersion.Cyclic dispersion occurs because the turbulence within the cylinder varies from cycle to cycle, the air/fuel mixture is not homogeneous (there may even be droplets of fuel present) and the exhaust gas residuals will not be fully mixed with the unburned charge.It is widely accepted that the early flame development can have a profound effect on the subsequent combustion.2. non-uniform work of cylindersIn a multi-cylinder engine, there can be significant differences in the combustion process and pressure development between the cylinders.Section 3 Abnormal combustion4.3.1 Surface ignition(1) post-ignitionSurface ignition is caused by the mixture igniting as a result of contact with a hot surface, such as an exhaust valve. Post ignition is often characterized by 'running-on'; that is, the engine continues to fire after the ignition has been switched off.(2)pre-ignitionIf the surface ignition occurs in advance of the spark, then it is called pre-ignition. Pre-ignition causes an increase in the compression work and this causes a reduction in power. Pre-ignition leads to higher peak pressures and this in turn can cause self-ignition.4.3.2 Self-ignition (detonation, knock)Self-ignition occurs when the pressure and temperature of the unburnt gas are such as to cause spontaneous ignition. The flame front propagates away from the sparking plug, and the unburnt (or ‘end’) gas is heated by radiation from the flame front and compressed as a result of the combustion process. If spontaneous ignition of the unburnt gas occurs, there is a rapid pressure rise which can be characterized by a ‘knocking’. The ‘knock’ is audible, caused by resonances of the combustion chamber walls. As a result of knocking, the thermal boundary layer at the combustion chamber walls can be destroyed. This causes increased heat transfer.4.3.3 The effects of operating factors on the combustion process(1)Mixture strengthWhen λ<0.8 and λ>1.2 :• Flame speed is slow, economical efficiency is bad• Incomplete combustion of fuel, HC e missionsWhen λ=1.03--1.1 :• Fuel burning completely, b e is the lowest• The temperature in cylinder is the highest and a rich air, a lot of NOx emissions.When λ=0.8--0.9 :•pz、Tz、Δp/Δφ、pe all reached the highest• Deflagration tend to i ncrease• Incomplete combustion, so the CO emissions increased dramatically (2)Spark advance angleDefinition: The crankshaft angle from spark ignition point to top dead centerCharacteristics: Corresponding to each working condition, there is a "best" ignition advance angle; the gasoline engine can get the largest power and minimum fuel consumption•Ignition angle is too large, compression work increases, and the peak pressure increase, knock becomes more possible• Combustion ignition too late, the peak pressure and temperature drop, heat loss increase, power and thermal efficiency are lower, but the knock tended to decrease, reducing NOx emissions(3)Rotate speedSpeed increases, the turbulence enhance in the cylinder, the flame speed is proportional to the speed increaseWhen speed increases, the knock tend to decrease, the ignition advance angle should be corresponding increase.(4)LoadGasoline engine load adjustment is volume adjustment,When load decrease, the proportion of residual gas relative increase, need to increase the ignition advance angle(5)Atmospheric conditionsAtmospheric pressure is low (plateau), cylinder charge reduce, economy and power performance decline, knock tend to decreaseAir temperature is high, cylinder charge fall too, prone to knock and gas resistanceSection 4 Combustion chamber in SI engines4.4.1 Conventional combustion chambersFor good fuel economy all the fuel should be burnt and the quench areas where the flame is extinguished should be minimized. The combustion chamber should have a low surface-to-volume ratio to minimize heat transfer.For high-performance engines, smaller cylinders will enable more rapid combustion, so permitting higher operating speeds and consequently greater power output.All these combustion chambers have:(i) short maximum flame travel(ii) the spark plug close to the exhaust valve (iii) a squish area to generate turbulence (iv) well-cooled end gas.。

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Chapter 2 Engine Gas Exchange ProcessesKey points: Gas exchange process of four-stroke internal combustion engine and ventilation losses, the concept of combustion engine filling coefficient.Difficult points: The measures to improve internal combustion engine filling quantity coefficient.2.1 Inlet and exhaust process of the four-stroke engineThe purpose of the exhaust and inlet processes or of the scavenging process is to remove the burned gases at the end of the power stroke and admit the fresh charge for the next cycle.Inducting the maximum air mass at wide-open throttle or full load and retaining that mass within the cylinder is the primary goal of the gas exchange processes.Engine gas exchange processes are characterized by overall parameters such as volumetric efficiency for four-stroke cycles.2.1.1 Gas exchange process of four-stroke engineThe gas exchange process of an engine consists of the duration from opening the exhaust valve to closing the inlet valve, it extends approximately 410~480ºCA and can be divided into four phases—blowdown, displacement, induction and scavenging.1.BlowdownThe duration from exhaust valve opening to cylinder pressure closes to pipe pressure is referred to as blowdown phase.The burned cylinder gases are discharged due to the pressure difference between the cylinder and the exhaust system. If the exhaust valve begins to open when the piston reached BDC, back pressure against the upward piston must be extremely high. Thus the exhaust process usually begins 40~60ºCA before BDC (exhaust lead crank angle).Blowdown phases ends when pressure difference between the cylinder and the exhaust system disappears, about 10~30ºCA after BDC. Though the free exhaust phase covers only about 1/10 of exhaust stroke, it discharges 60% of burned gas.2. DisplacementThe exhaust gas is scavenged by piston’s upward motion that is the burnt gas is forced out of the cylinder. It is a positive displace process.The exhaust valve closes 15~30ºCA after TDC (exhaust lag crank angle) to improve emptying the cylinders and make the best use of the inertia of the gases in the exhaust systems.3. Induction processFrom the inlet valves open to close, the whole process that internal combustion engine inhales fresh charge is called intake process.The usual practice is to extend the valve open phases beyond the intake strokes to improve charging of the cylinders and make the best use of the inertia of the gases in the intake systems.The intake valve opens 10~20ºCA before TDC (the inlet lead crank angle) and closes 40~70ºCA after BDC (the inlet lag crank angle).4. Valve overlap and scavengingThe exhaust valve closes 15 to 30ºCA after TDC and the inlet valve opens 10 to 20ºCA before TDC. The duration that both valves are open are called an overlap period.With both valves opening, the inertia of fresh charge can be used to sweep the exhaust gases out of cylinder without any loss if the overlap is proper, that is so called scavenging.The advantage of valve overlap occurs at high engine speeds when the longer valve-open periods improve volumetric efficiency. If the valve overlap is too large, backflow of exhausted gas into the cylinder gases into the intake will usually occur.2.1.2 Valve timingThe valve timing are modified to set better charging and exhausting performance as there is always a difference between theory and practical.2.2Volumetric efficiencyOne of the most important processes that govern how much power and performance can be obtained from an engine is getting the maximum amount of air into the cylinder during each cycle.1.Definition of volumetric efficiencyV olumetric efficiency is a measure of the effectiveness of the induction and exhaust processes.In terms of quantities applying to an actual engine, volumetric efficiency isdefined as the mass of fresh mixture which passes into the cylinder in one suction stroke, divided by the mass of this mixture which would fill the piston displacement at inlet density.ss a v V V m m 1==η (2.1) Where m a = mass of air inhaled per cylinder per cycle;m s = mass of air to occupy swept volume per cylinder at “ambient” pressure and temperature;V 1= volume of “ambient ” air inhaled per cylinder per cycle;V s = cylinder swept volume.2. The influence factors of volumetric efficiencyWhen inlet valve closed, the overall volume of cylinder is V s ’+V c , the mass of trapped working fluid is m a : a s c a V V m ρ)'(+= (2.2)Mass of residuals when exhaust valve closed: r r r V m ρ= (2.3)From (2.1),(2.2) and (2.3) ,fresh charges inhaled per cylinder per cycle is: ()r r a s c s s v V V V V ρρρη-+=' (2.4)Considering influence of intake and exhaust valve lag angle, make s c s c V V V V ++='ξ, c r V V =ϕ,then: )()1(1r a s v ϕρξερρεη--= (2.5) By applying Ideal Gas Equation )/(RT p =ρ to Eq.(2.5): )(11r r a a s s v T p T p p T ϕξεεη--=(2.6) The level of exhaust residuals trapped in the cylinder has a significant effect on the cycle-by-cycle variations in combustion, and the emissions of NO X . The residual coefficient γ is defined as mass of residual trapped in cylinder at the end of intake stroke, divided by mass of fresh charge inhaled in the intake stroke. It is used toevaluate the residual percentage of mixture in cylinder. From (2.3) and (2.4):ra r r c a a r c r r a s c r r s s v r V V V V V V V V m ρερϕξρρϕρξρϕρρρρηγ-=-=-+==)'( (2.7) By applying (2.6) to (2.7):γεεξη+-=111a a s s v T p p T In a qualitative analysis, volumetric efficiency ηv increases with:(1) Increasing mixture pressure at the end of intake stroke p a ;(2) Decreasing mixture temperature at the end of intake stroke T a ;(3) Reducing residual coefficient γ;(4) Increasing compression ratio ɛ;(5) Suitable valve parameters ξ and φ.2.3 Effect of operating conditions and design on volumetric efficiency1. Inlet Mach index:For convenience the ratio of the typical velocity to the inlet sonic velocity, u/α, is called the inlet Mach index. The gas velocity is chosen by the following equation: i i pp A C V A u =Where u= gas velocity through the inlet valve at smallest area;A p = piston area; V p = mean piston speed;A i = nominal intake valve opening area; C i = inlet valve flow coefficient. And: αααi p i i pi p C V D b C V A A uZ 2)(=== Where Z= inlet valve Mach index; α= inlet sonic velocity;b= cylinder diameter; D i = inlet valve diameter.From a great number of experiments, it could be seen that the maximum volumetric efficiency is obtainable for an inlet Mach number of 0.55. Therefore, engine designers must take care of this factor to get the maximum volumetric efficiency for their engines.2. Effect on intake system frictionDuring the intake stroke, due to friction in each part of the intake system, the pressure in the cylinder p c is less than the atmospheric pressure p atm by an amount dependent on the square of the speed.2j j c atm v k p p p p ρ∑=∑∆=-=∆Where k= the resistance coefficient for that component which depends on itsgeometric details; ρ= density of fresh air; v j= the local velocity.3.Effect of inhaled charge heatingDesigns which minimize the temperatures of inlet manifolds, inlet ports, inlet valves and valve seats are desirable. Improvement of heat conductivity between these parts and the coolant is effective in reducing temperature of fresh charge.4.Effect of speed and valve timingFlow effects on volumetric efficiency depend on the velocity of the fresh mixture in the intake manifold, port, and valve. Frictional flow losses increase as the square of engine speed, at higher engine speeds, the flow into the engine becomes choked.Earlier-than-normal inlet valve closing reduces back-flow losses at low speed and increases ηv. Later-than-normal inlet valve closing, results in a decreasing inη at low engine speeds due to backflow.v5.Effect of intake runner lengthThe high volumetric efficiencies can be obtained at certain speeds by means of long inlet pipes. The effects noted are caused by the inertia and elasticity of the gases in the inlet pipe and cylinder.As pipes become shorter, the maximum gains in volumetric efficiency grow smaller, but the range of speeds over which some gain is made grows wider.。

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