Direct Comparison of an Engine Working Under Otto, Miller and Diesel Cycles: Thermodynamic Analysis and Real Engine Performance
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Constant Volume Combustion Cycle for IC Engines
Constant Volume Combustion Cycle for IC Engines Jovan Dorić Assistant This paper presents an analysis of the internal combustion engine cycle in University of Novi Sad Faculty of Technical Sciences cases when the new unconventional piston motion law is used. The main goal of the presented unconventional piston motion law is to make a Ivan Klinar realization of combustion during constant volume in an engine’s cylinder. Full Professor The obtained results are shown in PV (pressure-volume) diagrams of University of Novi Sad Faculty of Technical Sciences standard and new engine cycles. The emphasis is placed on the shortcomings of the real cycle in IC engines as well as policies that would Marko Dorić contribute to reducing these disadvantages. For this paper, volumetric PhD student efficiency, pressure and temperature curves for standard and new piston University of Novi Sad Faculty of Agriculture motion law have been calculated. Also, the results of improved efficiency and power are presented. Keywords: constant volume combustion, IC engine, kinematics. 1. INTRODUCTION of an internal combustion engine, whose combustion is so rapid that the piston does not move during the Internal combustion engine simulation modelling has combustion process, and thus combustion is assumed to long been established as an effective tool for studying take place at constant volume [6]. Although in engine performance and contributing to evaluation and theoretical terms heat addition takes place at constant new developments. Thermodynamic models of the real volume, in real engine cycle heat addition at constant engine cycle have served as effective tools for complete volume can not be performed. -
Steady State and Transient Efficiencies of A
STEADY STATE AND TRANSIENT EFFICIENCIES OF A FOUR CYLINDER DIRECT INJECTION DIESEL ENGINE FOR IMPLEMENTATION IN A HYBRID ELECTRIC VEHICLE A Thesis Presented to The Graduate Faculty of The University of Akron In Partial Fulfillment of the Requirements for the Degree Masters of Science Charles Van Horn August, 2006 STEADY STATE AND TRANSIENT EFFICIENCIES OF A FOUR CYLINDER DIRECT INJECTION DIESEL ENGINE FOR IMPLEMENTATION IN A HYBRID ELECTRIC VEHICLE Charles Van Horn Thesis Approved: Accepted: Advisor Department Chair Dr. Scott Sawyer Dr. Celal Batur Faculty Reader Dean of the College Dr. Richard Gross Dr. George K. Haritos Faculty Reader Dean of the Graduate School Dr. Iqbal Husain Dr. George R. Newkome Date ii ABSTRACT The efficiencies of a four cylinder direct injection diesel engine have been investigated for the implementation in a hybrid electric vehicle (HEV). The engine was cycled through various operating points depending on the power and torque requirements for the HEV. The selected engine for the HEV is a 2005 Volkswagen 1.9L diesel engine. The 2005 Volkswagen 1.9L diesel engine was tested to develop the steady-state engine efficiencies and to evaluate the transient effects on these efficiencies. The peak torque and power curves were developed using a water brake dynamometer. Once these curves were obtained steady-state testing at various engine speeds and powers was conducted to determine engine efficiencies. Transient operation of the engine was also explored using partial throttle and variable throttle testing. The transient efficiency was compared to the steady-state efficiencies and showed a decrease from the steady- state values. -
Hybrid Electric Vehicles: a Review of Existing Configurations and Thermodynamic Cycles
Review Hybrid Electric Vehicles: A Review of Existing Configurations and Thermodynamic Cycles Rogelio León , Christian Montaleza , José Luis Maldonado , Marcos Tostado-Véliz * and Francisco Jurado Department of Electrical Engineering, University of Jaén, EPS Linares, 23700 Jaén, Spain; [email protected] (R.L.); [email protected] (C.M.); [email protected] (J.L.M.); [email protected] (F.J.) * Correspondence: [email protected]; Tel.: +34-953-648580 Abstract: The mobility industry has experienced a fast evolution towards electric-based transport in recent years. Recently, hybrid electric vehicles, which combine electric and conventional combustion systems, have become the most popular alternative by far. This is due to longer autonomy and more extended refueling networks in comparison with the recharging points system, which is still quite limited in some countries. This paper aims to conduct a literature review on thermodynamic models of heat engines used in hybrid electric vehicles and their respective configurations for series, parallel and mixed powertrain. It will discuss the most important models of thermal energy in combustion engines such as the Otto, Atkinson and Miller cycles which are widely used in commercial hybrid electric vehicle models. In short, this work aims at serving as an illustrative but descriptive document, which may be valuable for multiple research and academic purposes. Keywords: hybrid electric vehicle; ignition engines; thermodynamic models; autonomy; hybrid configuration series-parallel-mixed; hybridization; micro-hybrid; mild-hybrid; full-hybrid Citation: León, R.; Montaleza, C.; Maldonado, J.L.; Tostado-Véliz, M.; Jurado, F. Hybrid Electric Vehicles: A Review of Existing Configurations 1. Introduction and Thermodynamic Cycles. -
Development of Miller Cycle Gas Engine for Cogeneration
4. 9 & FR0105396 DEVELOPMENT OF MILLER CYCLE GAS ENGINE FOR COGENERATION DEVELOPPEMENT D UN MOTEUR A GAZ A CYCLE DE MILLER DESTINE A LA COGENERATION N. Tsukida , A.Sakakura, Y.Murata, and K. Okamoto Tokyo Gas CO.,LTD , Japan T.Abe and T. Takemoto Yanmar Diesel Engine CO.,LTD , Japan ABSTRACT We have developed a 300 kW gas engine cogeneration system for practical use that uses natural gas.Using a gas engine operated under conditions with an excess air ratio X =1 that is able to use a three way catalyst to purify the exhaust gases,we were able to achieve high efficiency through the application of the Miller Cycle, as well as a low NOx output. In terms of product specifications, we were able to achieve an electrical efficiency of 34.2% and a heat recovery efficiency of 49.3%, making an overall efficiency of 83.5% as a cogeneration system. RESUME Nous avons developpe un systeme de cogeneration de 300 kW avec moteur au gaz natural et tout a fait utilisable dans la pratique. Avec un moteur a gaz fonctionnant dans les conditions d ’un rapport d ’exces d ’air de X = 1 et capable d ’utiliser un catalyseur trois voies pour purifier les gaz d ’echappement, nous avons ete en mesure d ’obtenir un rendement eleve en appliquant le Cycle de Miller, et d ’obtenir egalement une faible emission d ’oxydes d ’azote. En termes de performances techniques du produit, nous avons obtenu un rendement electrique de 34,2 % et un rendement de recuperation thermique de 49,3 %, ce qui donne un rendement total de 83,5 % pour le systeme de cogeneration. -
Generation of Entropy in Spark Ignition Engines
Int. J. of Thermodynamics ISSN 1301-9724 Vol. 10 (No. 2), pp. 53-60, June 2007 Generation of Entropy in Spark Ignition Engines Bernardo Ribeiro, Jorge Martins*, António Nunes Universidade do Minho, Departamento de Engenharia Mecânica 4800-058 Guimarães PORTUGAL [email protected] Abstract Recent engine development has focused mainly on the improvement of engine efficiency and output emissions. The improvements in efficiency are being made by friction reduction, combustion improvement and thermodynamic cycle modification. New technologies such as Variable Valve Timing (VVT) or Variable Compression Ratio (VCR) are important for the latter. To assess the improvement capability of engine modifications, thermodynamic analysis of indicated cycles of the engines is made using the first and second laws of thermodynamics. The Entropy Generation Minimization (EGM) method proposes the identification of entropy generation sources and the reduction of the entropy generated by those sources as a method to improve the thermodynamic performance of heat engines and other devices. A computer model created and implemented in MATLAB Simulink was used to simulate the conventional Otto cycle and the various processes (combustion, free expansion during exhaust, heat transfer and fluid flow through valves and throttle) were evaluated in terms of the amount of the entropy generated. An Otto cycle, a Miller cycle (over-expanded cycle) and a Miller cycle with compression ratio adjustment are studied using the referred model in order to evaluate the amount of entropy generated in each cycle. All cycles are compared in terms of work produced per cycle. Keywords: IC engines, Miller cycle, entropy generation, over-expanded cycle 1. -
Thermodynamics of Power Generation
THERMAL MACHINES AND HEAT ENGINES Thermal machines ......................................................................................................................................... 1 The heat engine ......................................................................................................................................... 2 What it is ............................................................................................................................................... 2 What it is for ......................................................................................................................................... 2 Thermal aspects of heat engines ........................................................................................................... 3 Carnot cycle .............................................................................................................................................. 3 Gas power cycles ...................................................................................................................................... 4 Otto cycle .............................................................................................................................................. 5 Diesel cycle ........................................................................................................................................... 8 Brayton cycle ..................................................................................................................................... -
An Analytic Study of Applying Miller Cycle to Reduce Nox Emission from Petrol Engine Yaodong Wang, Lin Lin, Antony P
An analytic study of applying miller cycle to reduce nox emission from petrol engine Yaodong Wang, Lin Lin, Antony P. Roskilly, Shengchuo Zeng, Jincheng Huang, Yunxin He, Xiaodong Huang, Huilan Huang, Haiyan Wei, Shangping Li, et al. To cite this version: Yaodong Wang, Lin Lin, Antony P. Roskilly, Shengchuo Zeng, Jincheng Huang, et al.. An analytic study of applying miller cycle to reduce nox emission from petrol engine. Applied Thermal Engineering, Elsevier, 2007, 27 (11-12), pp.1779. 10.1016/j.applthermaleng.2007.01.013. hal-00498945 HAL Id: hal-00498945 https://hal.archives-ouvertes.fr/hal-00498945 Submitted on 9 Jul 2010 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Accepted Manuscript An analytic study of applying miller cycle to reduce nox emission from petrol engine Yaodong Wang, Lin Lin, Antony P. Roskilly, Shengchuo Zeng, Jincheng Huang, Yunxin He, Xiaodong Huang, Huilan Huang, Haiyan Wei, Shangping Li, J Yang PII: S1359-4311(07)00031-2 DOI: 10.1016/j.applthermaleng.2007.01.013 Reference: ATE 2070 To appear in: Applied Thermal Engineering Received Date: 5 May 2006 Revised Date: 2 January 2007 Accepted Date: 14 January 2007 Please cite this article as: Y. -
Heat Cycles, Heat Engines, & Real Devices
Heat Cycles, Heat Engines, & Real Devices John Jechura – [email protected] Updated: January 4, 2015 Topics • Heat engines / heat cycles . Review of ideal‐gas efficiency equations . Efficiency upper limit –Carnot Cycle • Water as working fluid in Rankine Cycle . Role of rotating equipment inefficiency • Advanced heat cycles . Reheat & heat recycle • Organic Rankine Cycle • Real devices . Gas & steam turbines 2 Heat Engines / Heat Cycles • Carnot cycle . Most efficient heat cycle possible Hot Reservoir @ T H • Rankine cycle Q H . Usually uses water (steam) as working fluid W . Creates the majority of electric power used net throughout the world Q C . Can use any heat source, including solar thermal, Cold Sink @ T coal, biomass, & nuclear C • Otto cycle . Approximates the pressure & volume of the combustion chamber of a spark‐ignited engine WQQ • Diesel cycle net H C th QQ . Approximates the pressure & volume of the HH combustion chamber of the Diesel engine 3 Carnot Cycle • Most efficient heat cycle possible • Steps . Reversible isothermal expansion of gas at TH. Combination of heat absorbed from hot reservoir & work done on the surroundings. Reversible isentropic & adiabatic expansion of the gas to TC. No heat transferred & work done on the surroundings. Reversible isothermal compression of gas at TC. Combination of heat released to cold sink & work done on the gas by the surroundings. Reversible isentropic & adiabatic compression of the gas to TH. No heat transferred & work done on the gas by the surroundings. • Thermal efficiency QQHC TT HC T C th th 1 QTTHHH 4 Rankine/Brayton Cycle • Different application depending on working fluid . Rankine cycle to describe closed steam cycle. -
Review of the Fundamentals Thermal Sciences
Review of the Fundamentals Reading Problems Review Chapter 3 and property tables More specifically, look at: 3.2 ! 3.4, 3.6, 3.7, 8.4, 8.5, 8.6, 8.8 Thermal Sciences The thermal sciences involve the storage, transfer and conversion of energy. Thermodynamics HeatTransfer Conservationofmass Conduction Conservationofenergy Convection Secondlawofthermodynamics Radiation HeatTransfer Properties Conjugate Thermal Thermodynamics Systems Engineering FluidsMechanics FluidMechanics Fluidstatics Conservationofmomentum Mechanicalenergyequation Modeling Thermodynamics: the study of energy, energy transformations and its relation to matter. The anal- ysis of thermal systems is achieved through the application of the governing conservation equations, namely Conservation of Mass, Conservation of Energy (1st law of thermodynam- ics), the 2nd law of thermodynamics and the property relations. Heat Transfer: the study of energy in transit including the relationship between energy, matter, space and time. The three principal modes of heat transfer examined are conduction, con- vection and radiation, where all three modes are affected by the thermophysical properties, geometrical constraints and the temperatures associated with the heat sources and sinks used to drive heat transfer. Fluid Mechanics: the study of fluids at rest or in motion. While this course will not deal exten- sively with fluid mechanics we will be influenced by the governing equations for fluid flow, namely Conservation of Momentum and Conservation of Mass. 1 Examples of Energy Conversion windmills -
3.5 the Internal Combustion Engine (Otto Cycle)
Thermodynamics and Propulsion Next: 3.6 Diesel Cycle Up: 3. The First Law Previous: 3.4 Refrigerators and Heat Contents Index Subsections 3.5.1 Efficiency of an ideal Otto cycle 3.5.2 Engine work, rate of work per unit enthalpy flux 3.5 The Internal combustion engine (Otto Cycle) [VW, S & B: 9.13] The Otto cycle is a set of processes used by spark ignition internal combustion engines (2-stroke or 4- stroke cycles). These engines a) ingest a mixture of fuel and air, b) compress it, c) cause it to react, thus effectively adding heat through converting chemical energy into thermal energy, d) expand the combustion products, and then e) eject the combustion products and replace them with a new charge of fuel and air. The different processes are shown in Figure 3.8: 1. Intake stroke, gasoline vapor and air drawn into engine ( ). 2. Compression stroke, , increase ( ). 3. Combustion (spark), short time, essentially constant volume ( ). Model: heat absorbed from a series of reservoirs at temperatures to . 4. Power stroke: expansion ( ). 5. Valve exhaust: valve opens, gas escapes. 6. ( ) Model: rejection of heat to series of reservoirs at temperatures to . 7. Exhaust stroke, piston pushes remaining combustion products out of chamber ( ). We model the processes as all acting on a fixed mass of air contained in a piston-cylinder arrangement, as shown in Figure 3.10. Figure 3.8: The ideal Otto cycle Figure 3.9: Sketch of an actual Otto cycle Figure 3.10: Piston and valves in a four-stroke internal combustion engine The actual cycle does not have the sharp transitions between the different processes that the ideal cycle has, and might be as sketched in Figure 3.9. -
Miller-Cycle on a Heavy Duty Diesel Engine
Miller-cycle on a heavy duty diesel engine Henrik Dembinski Clive Lewis Master of Science Thesis MMK 2009:1 MFM124 KTH Industrial Engineering and Management Machine Design SE-100 44 STOCKHOLM Master of Science Thesis MMK2 2009:1 MFM124 Miller-cycle on a heavy duty diesel engine Clive Lewis Henrik Dembinski Approved Examiner Supervisor 090128 Prof. Hans-Erik Ångström Prof. Hans-Erik Ångström Commissioner Contact person Scania CV AB Stefan Olsson 1. Sammanfattning Denna report beskriver ett examensarbete inom ämnet förbränningsmotorteknik och är utfört på Scania CV AB i Södertälje i sammarbete med Kungliga Tekniska Högskolan i Stockholm. Fordonsindustrin står inför nya utmaningar när en större fokusering på koldioxid (CO2) utsläpp från väg-gående fordon efterfrågas, vilket är direkt kopplat till fordonets bränsleförbrukning. Detta skall klaras av med lägre övriga emissioner i form av kväveoxider (NOx) och rök som är de två stora problemområdena för en dieselmotor. Scania vill därför undersöka potentialen med Miller cykling och om detta koncept skulle kunna implementeras på en lågeffektsmotor. Idén är att byta hög effekt mot verkningsgrad på motorer i motorprogrammet som inte utnyttjar hela grundmotorns effektpotential. Med Miller cykling menas senare- eller tidigarelagd stängning av insugsventilen och på så sätt öka graden expansionsarbete i förhållande till kompressionsarbete, dvs. öka den indikerade verkningsgraden. Då detta medför en minskning i effektiv slagvolym då cylindern inte fylls med luft helt måste kompensering i laddtryck göras för att motorn skall få samma luftmängd. En del kompressionsarbete görs då alltså utanför cylindern som belastar turbosystemet och inte motorn. En ny turbomatchning måste således göras då förflyttningar i turbomappen görs på ett mindre fördelaktigt sätt. -
Vation Is Left As an Cise
408 Chapter 9 Gas Power Systems 70 60 ~ I=" 50 ,:; u 40 'u"'" .....!.::: 30 0;" E 20 ~ ~ 10 0 5 10 15 20 .... Figure 9.6 Thermal efficiency of the cold air· Compression ralio, r standard Diesel cycle, k = 1.4. where r is the compression ratio and rc the cutoff ratio. The derivation is left as an cise. This relationship is shown in Fig. 9,6 for k = 1.4. Equation 9.13 for the Diesel differs from Eq. 9.8 for the Otto cycle only by the term in brackets, which for " > greater than unity. Thus, when the compression ratio is the same, the thermal the cold air-standard Diesel cycle would be less than that of the cold air-standard cycle. In the next example, we illustrate the analysis of the air-standard Diesel cycle. 1 II. I Q., ~ h 'I ....., ~',"1""": " .} ....I.-J,. l_ L ' ...... h,. "L b~ f .... l. Qt\VJ(",. / 'I".... tl.. ? r -J L...,.., U I'~J l.'''''/',; 1;1' J ... ,," j.,,>-I. '" At the beginning of the compression process of an air-standard Diesel cycle operating with a compression ratio of 18 , the perature is 300 K and the pressure is 0.1 MPa. The cutoC:( ratio for the cycle is 2. Determine (a) the temperature and at the end of each process of the cycle, (b) the thermal ' fficiency, (c) the mean effective pressure, in MPa. SOLUTION f'{UW ~ ' .... m c ..'( J ;(....clv4.. 'j ....;Y'\ j~..ll ~ ; ......'c.. Known: An air-standard Diesel cycle is executed with specified conditions at the beginning of the compression stroke.