Comparative Study of Different Organic Rankine Cycle Models: Simulations and Thermo-Economic Analysis for a Gas Engine Waste Heat Recovery Application
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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. -
Thermodynamic Optimization of an Organic Rankine Cycle for Power Generation from a Low Temperature Geothermal Heat Source
Thermodynamic Optimization of an Organic Rankine Cycle for Power Generation from a Low Temperature Geothermal Heat Source Inés Encabo Cáceres Roberto Agromayor Lars O. Nord Department of Energy and Process Engineering Norwegian University of Science and Technology (NTNU) Kolbjørn Hejes v.1B, NO-7491 Trondheim, Norway [email protected] Abstract fueled by natural gas or other fossil fuels (Macchi and Astolfi, 2017). However, during the last years, the The increasing concern on environment problems has increasing concern of the greenhouse effect and climate led to the development of renewable energy sources, change has led to an increase of renewable energy, such being the geothermal energy one of the most promising as wind and solar power. In addition to these listed ones in terms of power generation. Due to the low heat renewable energies, there is an energy source that shows source temperatures this energy provides, the use of a promising future due to the advantages it provides Organic Rankine Cycles is necessary to guarantee a when compared to other renewable energies. This good performance of the system. In this paper, the developing energy is geothermal energy, and its optimization of an Organic Rankine Cycle has been advantages are related to its availability (Macchi and carried out to determine the most suitable working fluid. Astolfi, 2017): it does not depend on the ambient Different cycle layouts and configurations for 39 conditions, it is stable, and it offers the possibility of different working fluids were simulated by means of a renewable energy base load operation. One of the Gradient Based Optimization Algorithm implemented challenges of geothermal energy is that it does not in MATLAB and linked to REFPROP property library. -
Transcritical Pressure Organic Rankine Cycle (ORC) Analysis Based on the Integrated-Average Temperature Difference in Evaporators
Applied Thermal Engineering 88 (2015) 2e13 Contents lists available at ScienceDirect Applied Thermal Engineering journal homepage: www.elsevier.com/locate/apthermeng Research paper Transcritical pressure Organic Rankine Cycle (ORC) analysis based on the integrated-average temperature difference in evaporators * Chao Yu, Jinliang Xu , Yasong Sun The Beijing Key Laboratory of Multiphase Flow and Heat Transfer for Low Grade Energy Utilizations, North China Electric Power University, Beijing 102206, PR China article info abstract Article history: Integrated-average temperature difference (DTave) was proposed to connect with exergy destruction (Ieva) Received 24 June 2014 in heat exchangers. Theoretical expressions were developed for DTave and Ieva. Based on transcritical Received in revised form pressure ORCs, evaporators were theoretically studied regarding DTave. An exact linear relationship be- 12 October 2014 tween DT and I was identified. The increased specific heats versus temperatures for organic fluid Accepted 11 November 2014 ave eva protruded its TeQ curve to decrease DT . Meanwhile, the decreased specific heats concaved its TeQ Available online 20 November 2014 ave curve to raise DTave. Organic fluid in the evaporator undergoes a protruded TeQ curve and a concaved T eQ curve, interfaced at the pseudo-critical temperature point. Elongating the specific heat increment Keywords: fi Organic Rankine Cycle section and shortening the speci c heat decrease section improved the cycle performance. Thus, the fi Integrated-average temperature difference system thermal and exergy ef ciencies were increased by increasing critical temperatures for 25 organic Exergy destruction fluids. Wet fluids had larger thermal and exergy efficiencies than dry fluids, due to the fact that wet fluids Thermal match shortened the superheated vapor flow section in condensers. -
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. -
Recording and Evaluating the Pv Diagram with CASSY
LD Heat Physics Thermodynamic cycle Leaflets P2.6.2.4 Hot-air engine: quantitative experiments The hot-air engine as a heat engine: Recording and evaluating the pV diagram with CASSY Objects of the experiment Recording the pV diagram for different heating voltages. Determining the mechanical work per revolution from the enclosed area. Principles The cycle of a heat engine is frequently represented as a closed curve in a pV diagram (p: pressure, V: volume). Here the mechanical work taken from the system is given by the en- closed area: W = − ͛ p ⋅ dV (I) The cycle of the hot-air engine is often described in an idealised form as a Stirling cycle (see Fig. 1), i.e., a succession of isochoric heating (a), isothermal expansion (b), isochoric cooling (c) and isothermal compression (d). This description, however, is a rough approximation because the working piston moves sinusoidally and therefore an isochoric change of state cannot be expected. In this experiment, the pV diagram is recorded with the computer-assisted data acquisition system CASSY for comparison with the real behaviour of the hot-air engine. A pressure sensor measures the pressure p in the cylinder and a displacement sensor measures the position s of the working piston, from which the volume V is calculated. The measured values are immediately displayed on the monitor in a pV diagram. Fig. 1 pV diagram of the Stirling cycle 0210-Wei 1 P2.6.2.4 LD Physics Leaflets Setup Apparatus The experimental setup is illustrated in Fig. 2. 1 hot-air engine . 388 182 1 U-core with yoke . -
Sustainable Energy Conversion Through the Use of Organic Rankine Cycles for Waste Heat Recovery and Solar Applications
ENERGY SYSTEMS RESEARCH UNIT AEROSPACE AND MECHANICAL ENGINEERING DEPARTMENT UNIVERSITY OF LIÈGE Sustainable Energy Conversion Through the Use of Organic Rankine Cycles for Waste Heat Recovery and Solar Applications. in Partial Fulfillment of the Requirements for the Degree of Doctor of Applied Sciences Presented to the Faculty of Applied Science of the University of Liège (Belgium) by Sylvain Quoilin Liège, October 2011 Introductory remarks Version 1.1, published in October 2011 © 2011 Sylvain Quoilin 〈►[email protected]〉 Licence. This work is licensed under the Creative Commons Attribution - No Derivative Works 2.5 License. To view a copy of this license, visit ►http://creativecommons.org/licenses/by-nd/2.5/ or send a letter to Creative Commons, 543 Howard Street, 5th Floor, San Francisco, California, 94105, USA. Contact the author to request other uses if necessary. Trademarks and service marks. All trademarks, service marks, logos and company names mentioned in this work are property of their respective owner. They are protected under trademark law and unfair competition law. The importance of the glossary. It is strongly recommended to read the glossary in full before starting with the first chapter. Hints for screen use. This work is optimized for both screen and paper use. It is recommended to use the digital version where applicable. It is a file in Portable Document Format (PDF) with hyperlinks for convenient navigation. All hyperlinks are marked with link flags (►). Hyperlinks in diagrams might be marked with colored borders instead. Navigation aid for bibliographic references. Bibliographic references to works which are publicly available as PDF files mention the logical page number and an offset (if non-zero) to calculate the physical page number. -
Section 15-6: Thermodynamic Cycles
Answer to Essential Question 15.5: The ideal gas law tells us that temperature is proportional to PV. for state 2 in both processes we are considering, so the temperature in state 2 is the same in both cases. , and all three factors on the right-hand side are the same for the two processes, so the change in internal energy is the same (+360 J, in fact). Because the gas does no work in the isochoric process, and a positive amount of work in the isobaric process, the First Law tells us that more heat is required for the isobaric process (+600 J versus +360 J). 15-6 Thermodynamic Cycles Many devices, such as car engines and refrigerators, involve taking a thermodynamic system through a series of processes before returning the system to its initial state. Such a cycle allows the system to do work (e.g., to move a car) or to have work done on it so the system can do something useful (e.g., removing heat from a fridge). Let’s investigate this idea. EXPLORATION 15.6 – Investigate a thermodynamic cycle One cycle of a monatomic ideal gas system is represented by the series of four processes in Figure 15.15. The process taking the system from state 4 to state 1 is an isothermal compression at a temperature of 400 K. Complete Table 15.1 to find Q, W, and for each process, and for the entire cycle. Process Special process? Q (J) W (J) (J) 1 ! 2 No +1360 2 ! 3 Isobaric 3 ! 4 Isochoric 0 4 ! 1 Isothermal 0 Entire Cycle No 0 Table 15.1: Table to be filled in to analyze the cycle. -
Thermodynamic Cycles of Direct and Pulsed-Propulsion Engines - V
THERMAL TO MECHANICAL ENERGY CONVERSION: ENGINES AND REQUIREMENTS – Vol. I - Thermodynamic Cycles of Direct and Pulsed-Propulsion Engines - V. B. Rutovsky THERMODYNAMIC CYCLES OF DIRECT AND PULSED- PROPULSION ENGINES V. B. Rutovsky Moscow State Aviation Institute, Russia. Keywords: Thermodynamics, air-breathing engine, turbojet. Contents 1. Cycles of Piston Engines of Internal Combustion. 2. Jet Engines Using Liquid Oxidants 3. Compressor-less Air-Breathing Jet Engines 3.1. Ramjet engine (with fuel combustion at p = const) 4. Pulsejet Engine. 5. Cycles of Gas-Turbine Propulsion Systems with Fuel Combustion at a Constant Volume Glossary Bibliography Summary This chapter considers engines with intermittent cycles and cycles of pulsejet engines. These include, piston engines of various designs, pulsejet engines, and gas-turbine propulsion systems with fuel combustion at a constant volume. This chapter presents thermodynamic cycles of thermal engines in which the propulsive mass is a mixture of air and either a gaseous fuel or vapor of a liquid fuel (on the initial portion of the cycle), and gaseous combustion products (over the rest of the cycle). 1. Cycles of Piston Engines of Internal Combustion. Piston engines of internal combustion are utilized in motor vehicles, aircraft, ships and boats, and locomotives. They are also used in stationary low-power electric generators. Given the variety of conditions that engines of internal combustion should meet, depending on their functions, engines of various types have been designed. From the standpointUNESCO of thermodynamics, however, – i.e. EOLSS in terms of operating cycles of these engines, all of them can be classified into three groups: (a) engines using cycles with heat addition at a constant volume (V = const); (b) engines using cycles with heat addition at a constantSAMPLE pressure (p = const); andCHAPTERS (c) engines using the so-called mixed cycles, in which heat is added at either a constant volume or a constant pressure. -
Thermodynamic Analysis of Solar Absorption Cooling System Open Access Jasim Abdulateef1,, Sameer Dawood Ali1, Mustafa Sabah Mahdi2
Journal of Advanced Research in Fluid Mechanics and Thermal Sciences 60, Issue 2 (2019) 233-246 Journal of Advanced Research in Fluid Mechanics and Thermal Sciences Journal homepage: www.akademiabaru.com/arfmts.html ISSN: 2289-7879 Thermodynamic Analysis of Solar Absorption Cooling System Open Access Jasim Abdulateef1,, Sameer Dawood Ali1, Mustafa Sabah Mahdi2 1 Mechanical Engineering Department, University of Diyala, 32001 Diyala, Iraq 2 Chemical Engineering Department, University of Diyala, 32001 Diyala, Iraq ARTICLE INFO ABSTRACT Article history: This study deals with thermodynamic analysis of solar assisted absorption refrigeration Received 16 April 2019 system. A computational routine based on entropy generation was written in MATLAB Received in revised form 14 May 2019 to investigate the irreversible losses of individual component and the total entropy Accepted 18 July 2018 generation (푆̇ ) of the system. The trend in coefficient of performance COP and 푆̇ Available online 28 August 2019 푡표푡 푡표푡 with the variation of generator, evaporator, condenser and absorber temperatures and heat exchanger effectivenesses have been presented. The results show that, both COP and Ṡ tot proportional with the generator and evaporator temperatures. The COP and irreversibility are inversely proportional to the condenser and absorber temperatures. Further, the solar collector is the largest fraction of total destruction losses of the system followed by the generator and absorber. The maximum destruction losses of solar collector reach up to 70% and within the range 6-14% in case of generator and absorber. Therefore, these components require more improvements as per the design aspects. Keywords: Refrigeration; absorption; solar collector; entropy generation; irreversible losses Copyright © 2019 PENERBIT AKADEMIA BARU - All rights reserved 1. -
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.