Stirling Machine Basics
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Jean-Baptiste Charles Joseph Bélanger (1790-1874), the Backwater Equation and the Bélanger Equation
THE UNIVERSITY OF QUEENSLAND DIVISION OF CIVIL ENGINEERING REPORT CH69/08 JEAN-BAPTISTE CHARLES JOSEPH BÉLANGER (1790-1874), THE BACKWATER EQUATION AND THE BÉLANGER EQUATION AUTHOR: Hubert CHANSON HYDRAULIC MODEL REPORTS This report is published by the Division of Civil Engineering at the University of Queensland. Lists of recently-published titles of this series and of other publications are provided at the end of this report. Requests for copies of any of these documents should be addressed to the Civil Engineering Secretary. The interpretation and opinions expressed herein are solely those of the author(s). Considerable care has been taken to ensure accuracy of the material presented. Nevertheless, responsibility for the use of this material rests with the user. Division of Civil Engineering The University of Queensland Brisbane QLD 4072 AUSTRALIA Telephone: (61 7) 3365 3619 Fax: (61 7) 3365 4599 URL: http://www.eng.uq.edu.au/civil/ First published in 2008 by Division of Civil Engineering The University of Queensland, Brisbane QLD 4072, Australia © Chanson This book is copyright ISBN No. 9781864999211 The University of Queensland, St Lucia QLD JEAN-BAPTISTE CHARLES JOSEPH BÉLANGER (1790-1874), THE BACKWATER EQUATION AND THE BÉLANGER EQUATION by Hubert CHANSON Professor, Division of Civil Engineering, School of Engineering, The University of Queensland, Brisbane QLD 4072, Australia Ph.: (61 7) 3365 3619, Fax: (61 7) 3365 4599, Email: [email protected] Url: http://www.uq.edu.au/~e2hchans/ REPORT No. CH69/08 ISBN 9781864999211 Division of Civil Engineering, The University of Queensland August 2008 Jean-Baptiste BÉLANGER (1790-1874) (Courtesy of the Bibliothèque de l'Ecole Nationale Supérieure des Ponts et Chaussées) Abstract In an open channel, the transition from a high-velocity open channel flow to a fluvial motion is a flow singularity called a hydraulic jump. -
Thermodynamic Analysis of GM-Type Pulse Tube Coolers Q Y.L
Cryogenics 41 &2001) 513±520 www.elsevier.com/locate/cryogenics Thermodynamic analysis of GM-type pulse tube coolers q Y.L. Ju *,1 Cryogenic Laboratory, Chinese Academy of Sciences, P.O. Box 2711, Beijing 100080, People's Republic of China Received 29 January 2001; accepted 28 June 2001 Abstract The thermodynamic loss of rotary valve and the coecient of performance &COP) of GM-type pulse tube coolers &PTCs) are discussed and explained by using the ®rst and second laws of thermodynamics in this paper. The COP of GM-type PTC, based on two types of pressure pro®les, the sinusoidal wave inside the pulse tube and the step wave at the compressor side, has been derived and compared with that of Stirling-type PTC. Result shows that additional compressor work is needed due to the irreversible entropy productions in the rotary valve thereby decreasing the COP of GM-type PTC. The eect of double-inlet mode on the COP of PTC has distinct improvement at lower temperature region &larger TH=TL). It is also shown that the COP of GM-type PTC is independent of the shape of the pressure pro®les in the ideal case of no ¯ow resistance in the regenerator. Ó 2001 Elsevier Science Ltd. All rights reserved. Keywords: Pulse tube cooler; GM-type; Thermodynamic analysis 1. Introduction achieved [13]. All these machines use a compressor and a valve system to produce pressure oscillation in the In general pulse tube cooler &PTC) requires a phase cooler system. They are called GM-type PTCs. shifter system, located at the hot end of the pulse tube, A GM-type PTC, shown in Fig. -
Converting an Internal Combustion Engine Vehicle to an Electric Vehicle
AC 2011-1048: CONVERTING AN INTERNAL COMBUSTION ENGINE VEHICLE TO AN ELECTRIC VEHICLE Ali Eydgahi, Eastern Michigan University Dr. Eydgahi is an Associate Dean of the College of Technology, Coordinator of PhD in Technology program, and Professor of Engineering Technology at the Eastern Michigan University. Since 1986 and prior to joining Eastern Michigan University, he has been with the State University of New York, Oak- land University, Wayne County Community College, Wayne State University, and University of Maryland Eastern Shore. Dr. Eydgahi has received a number of awards including the Dow outstanding Young Fac- ulty Award from American Society for Engineering Education in 1990, the Silver Medal for outstanding contribution from International Conference on Automation in 1995, UNESCO Short-term Fellowship in 1996, and three faculty merit awards from the State University of New York. He is a senior member of IEEE and SME, and a member of ASEE. He is currently serving as Secretary/Treasurer of the ECE Division of ASEE and has served as a regional and chapter chairman of ASEE, SME, and IEEE, as an ASEE Campus Representative, as a Faculty Advisor for National Society of Black Engineers Chapter, as a Counselor for IEEE Student Branch, and as a session chair and a member of scientific and international committees for many international conferences. Dr. Eydgahi has been an active reviewer for a number of IEEE and ASEE and other reputedly international journals and conferences. He has published more than hundred papers in refereed international and national journals and conference proceedings such as ASEE and IEEE. Mr. Edward Lee Long IV, University of Maryland, Eastern Shore Edward Lee Long IV graduated from he University of Maryland Eastern Shore in 2010, with a Bachelors of Science in Engineering. -
Physics 170 - Thermodynamic Lecture 40
Physics 170 - Thermodynamic Lecture 40 ! The second law of thermodynamic 1 The Second Law of Thermodynamics and Entropy There are several diferent forms of the second law of thermodynamics: ! 1. In a thermal cycle, heat energy cannot be completely transformed into mechanical work. ! 2. It is impossible to construct an operational perpetual-motion machine. ! 3. It’s impossible for any process to have as its sole result the transfer of heat from a cooler to a hotter body ! 4. Heat flows naturally from a hot object to a cold object; heat will not flow spontaneously from a cold object to a hot object. ! ! Heat Engines and Thermal Pumps A heat engine converts heat energy into work. According to the second law of thermodynamics, however, it cannot convert *all* of the heat energy supplied to it into work. Basic heat engine: hot reservoir, cold reservoir, and a machine to convert heat energy into work. Heat Engines and Thermal Pumps 4 Heat Engines and Thermal Pumps This is a simplified diagram of a heat engine, along with its thermal cycle. Heat Engines and Thermal Pumps An important quantity characterizing a heat engine is the net work it does when going through an entire cycle. Heat Engines and Thermal Pumps Heat Engines and Thermal Pumps Thermal efciency of a heat engine: ! ! ! ! ! ! From the first law, it follows: Heat Engines and Thermal Pumps Yet another restatement of the second law of thermodynamics: No cyclic heat engine can convert its heat input completely to work. Heat Engines and Thermal Pumps A thermal pump is the opposite of a heat engine: it transfers heat energy from a cold reservoir to a hot one. -
Internal and External Combustion Engine Classifications: Gasoline
Internal and External Combustion Engine Classifications: Gasoline and diesel engine classifications: A gasoline (Petrol) engine or spark ignition (SI) burns gasoline, and the fuel is metered into the intake manifold. Spark plug ignites the fuel. A diesel engine or (compression ignition Cl) bums diesel oil, and the fuel is injected right into the engine combustion chamber. When fuel is injected into the cylinder, it self ignites and bums. Preparation of fuel air mixture (gasoline engine): * High calorific value: (Benzene (Gasoline) 40000 kJ/kg, Diesel 45000 kJ/kg). * Air-fuel ratio: A chemically correct air-fuel ratio is called stoichiometric mixture. It is an ideal ratio of around 14.7:1 (14.7 parts of air to 1 part fuel by weight). Under steady-state engine condition, this ratio of air to fuel would assure that all of the fuel will blend with all of the air and be burned completely. A lean fuel mixture containing a lot of air compared to fuel, will give better fuel economy and fewer exhaust emissions (i.e. 17:1). A rich fuel mixture: with a larger percentage of fuel, improves engine power and cold engine starting (i.e. 8:1). However, it will increase emissions and fuel consumption. * Gasoline density = 737.22 kg/m3, air density (at 20o) = 1.2 kg/m3 The ratio 14.7 : 1 by weight equal to 14.7/1.2 : 1/737.22 = 12.25 : 0.0013564 The ratio is 9,030 : 1 by volume (one liter of gasoline needs 9.03 m3 of air to have complete burning). -
Midlothian Council the Moray Council Perth & Kinross Council South
1558 THE EDINBURGH GAZETTE FRIDAY 23 JULY 1999 Glenferness Proposed demolition Area Planning Office Reason for advert Application House of link corridor. 88 High Street and period for response Auldearn 99/00104/LBCNA Nairn IV124BD Listed Building Consent 99/01057/PPLB IV2 SUP Environmental and Erection of manager's house Consumer Services (in outline) on site at Ballintulm / D Rennilson, Director of Planning & Development (1601/86) 46 Leslie Street, Blairgowrie Caravan Park, Ballintulm, (21 days) Blairgowrie, Perthshire for Ballintulm Caravan Park. Midlothian Council Listed Building Consent 99/01077/LBC (21 days) Installation of sash and case windows The following application may be examined at the Community Services at Sealsbridge House, Back Street, Division, Fairfield House, 8 Lothian Road, Dalkeith EH22 3ZQ, from Bridge of Earn, Perth PH2 9AE for 9.1Sam to 4.45pm Mondays to Thursdays and from 9.15am to 3.30pm, LShaw Fridays or in the local library as indicated. Listed Building Consent 99/01098/LBC LISTED BUILDING CONSENT Environmental and Re-paint existing render at 99/00397/LBC Consumer Services Howgait, Lochgelly Road, Greenfield Lodge Erection of conservatory and alterations to 21/25 High Street, Kinross Scotlandwell, Kinross KY13 9JA Lasswade dwellinghouse. (21 days) for Dr and Mrs E Carruthers Midlothian .Local library: Bonnyrigg Listed Building Consent 99/01120/PPLB Environmental and Alterations and extension to house 'Please send any comment to me in writing not later than 13th August Consumer Services at Tirinie House, Glenfender 1999. 26 Atholl Road, Pitlochry Blair Atholl, Pitlochry G W Marwick, Director; Community Services (1601/72) (21 days) Perthshire PH185TU for Mr and Mrs D Profumo. -
Abstract 1. Introduction 2. Robert Stirling
Stirling Stuff Dr John S. Reid, Department of Physics, Meston Building, University of Aberdeen, Aberdeen AB12 3UE, Scotland Abstract Robert Stirling’s patent for what was essentially a new type of engine to create work from heat was submitted in 1816. Its reception was underwhelming and although the idea was sporadically developed, it was eclipsed by the steam engine and, later, the internal combustion engine. Today, though, the environmentally favourable credentials of the Stirling engine principles are driving a resurgence of interest, with modern designs using modern materials. These themes are woven through a historically based narrative that introduces Robert Stirling and his background, a description of his patent and the principles behind his engine, and discusses the now popular model Stirling engines readily available. These topical models, or alternatives made ‘in house’, form a good platform for investigating some of the thermodynamics governing the performance of engines in general. ---------------------------------------------------------------------------------------------------------------- 1. Introduction 2016 marks the bicentenary of the submission of Robert Stirling’s patent that described heat exchangers and the technology of the Stirling engine. James Watt was still alive in 1816 and his steam engine was gaining a foothold in mines, in mills, in a few goods railways and even in pioneering ‘steamers’. Who needed another new engine from another Scot? The Stirling engine is a markedly different machine from either the earlier steam engine or the later internal combustion engine. For reasons to be explained, after a comparatively obscure two centuries the Stirling engine is attracting new interest, for it has environmentally friendly credentials for an engine. This tribute introduces the man, his patent, the engine and how it is realised in example models readily available on the internet. -
MODELING and ANALYSIS of PULSE TUBE REFRIGERATOR 1Nishant Solanki, 2Nimesh Parmar
Solanki et al., International Journal of Advanced Engineering Technology E-ISSN 0976-3945 Research Paper MODELING AND ANALYSIS OF PULSE TUBE REFRIGERATOR 1Nishant Solanki, 2Nimesh Parmar Address for Correspondence 1Student, M.E. (Thermal Engineering), Gandhinagar Institute of Technology, Gandhinagar, Gujarat, India 2Asst. Professor, Mechanical Engineering Department, Gandhinagar Institute of Technology, Gandhinagar, Gujarat, India ABSTRACT: Cryogenics comes from the Greek word “kryos”, which means very cold or freezing and “genes” means to produce. Cryogenics is the science and technology associated with the phenomena that occur at very low temperature, close to the lowest theoretically attainable temperature. In this research paper, three dimensional model of pulse tube refrigerator is developed in ANSYS CFX and compared it with experimental results. It shows good agreement with experimental results with ANSYS CFD results. KEYWORDS : Pulse tube refrigerator, ANSYS CFD INTRODUCTION: volume on the thermodynamic performance of The pulse tube refrigerators (PTR) are capable of various components in a simple orifice and a double cooling to temperature below 123K. Unlike the inlet pulse tube cooler by combining a linearized ordinary refrigeration cycles which utilize the vapour model with a thermodynamic analysis. The results compression cycle as described in classical reveal that the performance of the pulse tube cooler is thermodynamics, a PTR implements the theory of significantly affected when the reservoir to pulse tube oscillatory compression and expansion of the gas volume ratio is less than 5, which helps the design of within a closed volume to achieve desired a practical pulse tube cooler. refrigeration. Being oscillatory, a PTR is a non steady Y.L. He, C.F. -
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 . -
William Stirling
William Stirling William Stirling was born 31 August 1841 in Forfar, Angus, Scotland. He was the second of eight children of Thomas Stirling and Elizabeth Bell, three of whom died young. In 1851, the family was living in Forfar, Scotland.1 William joined the Mormon Church in 1859.2 He was a ploughman living in Inverarity, Angus, Scotland, in 1861.3 The next year he sailed with his sister Jessie from Liverpool, England, to New York, United States, on the ship “William Tapscott”. They arrived 26 June 1862.4 They continued to the Utah Territory with the Horton D Haight Company, departing 10 August 1862 and arriving19 October 1862.5 William drove an ox team across the plains. He moved to Dixie in December 1862.6 He became a naturalized citizen.7 William married Sarah Ann Leany in 1865 in Harrisburg, Washington, Utah Territory.8 They had fourteen children.9 He built a small two-room lumber house in 1868 in Leeds, Washington, Utah Territory (the Stirling-Olsen home). He helped fund his parents and two younger sisters to immigrate to Great Salt Lake City. He was a farmer, winemaker, and the chief executive officer for the Leeds Water Company. One winter he was riding his horse through Silver Reef (a silver mining town near Leeds) and noticed a frenzy at the Christy Mill. The boilers were under full fire, but the mill stream was frozen. Knowing an explosion was inevitable if the water was unavailable to cool the mill, he quickly rode to open the head gates which directed water from the Leeds Canal.10 The owners showed their gratitude by placing William on the payroll for a year with no expectation that he would work for the salary. -
Novel Hot Air Engine and Its Mathematical Model – Experimental Measurements and Numerical Analysis
POLLACK PERIODICA An International Journal for Engineering and Information Sciences DOI: 10.1556/606.2019.14.1.5 Vol. 14, No. 1, pp. 47–58 (2019) www.akademiai.com NOVEL HOT AIR ENGINE AND ITS MATHEMATICAL MODEL – EXPERIMENTAL MEASUREMENTS AND NUMERICAL ANALYSIS 1 Gyula KRAMER, 2 Gabor SZEPESI *, 3 Zoltán SIMÉNFALVI 1,2,3 Department of Chemical Machinery, Institute of Energy and Chemical Machinery University of Miskolc, Miskolc-Egyetemváros 3515, Hungary e-mail: [email protected], [email protected], [email protected] Received 11 December 2017; accepted 25 June 2018 Abstract: In the relevant literature there are many types of heat engines. One of those is the group of the so called hot air engines. This paper introduces their world, also introduces the new kind of machine that was developed and built at Department of Chemical Machinery, Institute of Energy and Chemical Machinery, University of Miskolc. Emphasizing the novelty of construction and the working principle are explained. Also the mathematical model of this new engine was prepared and compared to the real model of engine. Keywords: Hot, Air, Engine, Mathematical model 1. Introduction There are three types of volumetric heat engines: the internal combustion engines; steam engines; and hot air engines. The first one is well known, because it is on zenith nowadays. The steam machines are also well known, because their time has just passed, even the elder ones could see those in use. But the hot air engines are forgotten. Our aim is to consider that one. The history of hot air engines is 200 years old. -
Assessing the Evolution of the Airborne Generation of Thermal Lift in Aerostats 1783 to 1883
Journal of Aviation/Aerospace Education & Research Volume 13 Number 1 JAAER Fall 2003 Article 1 Fall 2003 Assessing the Evolution of the Airborne Generation of Thermal Lift in Aerostats 1783 to 1883 Thomas Forenz Follow this and additional works at: https://commons.erau.edu/jaaer Scholarly Commons Citation Forenz, T. (2003). Assessing the Evolution of the Airborne Generation of Thermal Lift in Aerostats 1783 to 1883. Journal of Aviation/Aerospace Education & Research, 13(1). https://doi.org/10.15394/ jaaer.2003.1559 This Article is brought to you for free and open access by the Journals at Scholarly Commons. It has been accepted for inclusion in Journal of Aviation/Aerospace Education & Research by an authorized administrator of Scholarly Commons. For more information, please contact [email protected]. Forenz: Assessing the Evolution of the Airborne Generation of Thermal Lif Thermal Lift ASSESSING THE EVOLUTION OF THE AIRBORNE GENERATION OF THERMAL LIFT IN AEROSTATS 1783 TO 1883 Thomas Forenz ABSTRACT Lift has been generated thermally in aerostats for 219 years making this the most enduring form of lift generation in lighter-than-air aviation. In the United States over 3000 thermally lifted aerostats, commonly referred to as hot air balloons, were built and flown by an estimated 12,000 licensed balloon pilots in the last decade. The evolution of controlling fire in hot air balloons during the first century of ballooning is the subject of this article. The purpose of this assessment is to separate the development of thermally lifted aerostats from the general history of aerostatics which includes all gas balloons such as hydrogen and helium lifted balloons as well as thermally lifted balloons.