Low-Temperature-Differential) Heat Engine
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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. -
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. -
Physics 100 Lecture 7
2 Physics 100 Lecture 7 Heat Engines and the 2nd Law of Thermodynamics February 12, 2018 3 Thermal Convection Warm fluid is less dense and rises while cool fluid sinks Resulting circulation efficiently transports thermal energy 4 COLD Convection HOT Turbulent motion of glycerol in a container heated from below and cooled from above. The bright lines show regions of rapid temperature variation. The fluid contains many "plumes," especially near the walls. The plumes can be identified as mushroom-shaped objects with heat flowing through the "stalk" and spreading in the "cap." The hot plumes tend to rise with their caps on top; falling, cold plumes are cap-down. All this plume activity is carried along in an overall counterclockwise "wind" caused by convection. Note the thermometer coming down from the top of the cell. Figure adapted from J. Zhang, S. Childress, A. Libchaber, Phys. Fluids 9, 1034 (1997). See detailed discussion in Kadanoff, L. P., Physics Today 54, 34 (August 2001). 5 The temperature of land changes more quickly than the nearby ocean. Thus convective “sea breezes” blow ____ during the day and ____ during the night. A. onshore … onshore B. onshore … offshore C. offshore … onshore D. offshore … offshore 6 The temperature of land changes more quickly than the nearby ocean. Thus convective “sea breezes” blow ____ during the day and ____ during the night. A. onshore … onshore B.onshore … offshore C.offshore … onshore D.offshore … offshore 7 Thermal radiation Any object whose temperature is above zero Kelvin emits energy in the form of electromagnetic radiation Objects both absorb and emit EM radiation continuously, and this phenomenon helps determine the object’s equilibrium temperature 8 The electromagnetic spectrum 9 Thermal radiation We’ll examine this concept some more in chapter 6 10 Why does the Earth cool more quickly on clear nights than it does on cloudy nights? A. -
Feasibility Study Into Stirling Engines Application in Ship's Energy Systems
Transactions on the Built Environment vol 42, © 1999 WIT Press, www.witpress.com, ISSN 1743-3509 Feasibility study into Stirling engines application in ship's energy systems S. Zmudzki, Faculty of Maritime Technology, Technical University of Szczecin, 71- 065 Szczecin, al Piastow 41, Poland E-mail: szmudzkia@shiptech. tuniv.szczecin.pl Abstract The possibility of utilization of solar energy as well as exhaust gas energy from main and auxiliary marine diesel engines for driving Stirling engines has been analysed. The Stirling engines are used for driving current generators. The solar dish Stirling units of 100 kW total effective power may be installed on a board of different type of ships. The system utilizing the exhaust gas energy has been provided with three-way catalyst which may lead to the reduction of emissions below limits established by appropriate regulations. 1 Introduction The Stirling engine belongs to a group of piston engines with so called external supply of heat energy, flowing then through metal walls of engine heater into working gas circulating in the working space. The heat energy supply may be realized or by means of direct effect of the high temperature energy source or by an intermediate heating system i.e. heat pipe or pool-boiler receiver. Thus, the design provides for the possibility of application of different types of heat energy of sufficiently large power. In particular, the advantages of Stirling engines are set off when using the alternative energy sources, especially waste heat energy, the operating costs for which are relatively lower in comparison with capital costs. In case of ship s energy installations, the solar energy available at appropriate geographical latitudes for ships having very large open deck surface / i.e. -
Fuel Cells Versus Heat Engines: a Perspective of Thermodynamic and Production
Fuel Cells Versus Heat Engines: A Perspective of Thermodynamic and Production Efficiencies Introduction: Fuel Cells are being developed as a powering method which may be able to provide clean and efficient energy conversion from chemicals to work. An analysis of their real efficiencies and productivity vis. a vis. combustion engines is made in this report. The most common mode of transportation currently used is gasoline or diesel engine powered automobiles. These engines are broadly described as internal combustion engines, in that they develop mechanical work by the burning of fossil fuel derivatives and harnessing the resultant energy by allowing the hot combustion product gases to expand against a cylinder. This arrangement allows for the fuel heat release and the expansion work to be performed in the same location. This is in contrast to external combustion engines, in which the fuel heat release is performed separately from the gas expansion that allows for mechanical work generation (an example of such an engine is steam power, where fuel is used to heat a boiler, and the steam then drives a piston). The internal combustion engine has proven to be an affordable and effective means of generating mechanical work from a fuel. However, because the majority of these engines are powered by a hydrocarbon fossil fuel, there has been recent concern both about the continued availability of fossil fuels and the environmental effects caused by the combustion of these fuels. There has been much recent publicity regarding an alternate means of generating work; the hydrogen fuel cell. These fuel cells produce electric potential work through the electrochemical reaction of hydrogen and oxygen, with the reaction product being water. -
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 . -
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. -
Measuring the Steady State Thermal Efficiency of a Heating System
Measuring the Steady State Thermal Efficiency of a Heating System. Last week you had a tour of “Colby Power and Light” and had a chance to see Gus Libby’s really cool, campus-scale, multi-million dollar calorimeter. This week we will use lab-scale calorimeters to measure the heat and carbon content of different fuels (methane, propane, butane, and gasoline). Our simple calorimeters were designed by Whitney King and Chuck Jones, Science Division Instrument Wizard, to simulate the highly efficient HTP Versa Flame fire-tube boiler. The lab has three parts: 1) Calibrate the calorimeter 2) Measure the heat content of different fuels 3) Compare the measured heat content to the calculated heat content 1) Calibrate the Calorimeter. You lab instructor will demonstrate the assembly of the laboratory- scale fire-tube calorimeter. The heat transferred from the burning fuel to the calorimeter can be determined from the mass of the object being heated, the heat capacity of the object and the change in temperature. � = ���� ∗ �� ∗ ∆� We will begin the experiment by adding a known amount of heat to our calorimeters from a coffee cup heater. The heater is a simple resistor that converts electrical energy into heat. The heater has a resistance of 47.5 ohms and is plugged into a 120 V outlet. Recalling your electricity basics, we know that V=IR where V is the voltage in Figure 1. HTP Versa Flame Fire Tube volts, I is the current in amps, and R is the Boiler. Brown Tubes carry the hot resistance in ohms. The power, P, consumed by combustion gasses inside of the the heater is volts times current, water tank where they condense releasing the maximum available 2 heat. -
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 ..................................................................................................................................... -
Power Plant Steam Cycle Theory - R.A
THERMAL POWER PLANTS – Vol. I - Power Plant Steam Cycle Theory - R.A. Chaplin POWER PLANT STEAM CYCLE THEORY R.A. Chaplin Department of Chemical Engineering, University of New Brunswick, Canada Keywords: Steam Turbines, Carnot Cycle, Rankine Cycle, Superheating, Reheating, Feedwater Heating. Contents 1. Cycle Efficiencies 1.1. Introduction 1.2. Carnot Cycle 1.3. Simple Rankine Cycles 1.4. Complex Rankine Cycles 2. Turbine Expansion Lines 2.1. T-s and h-s Diagrams 2.2. Turbine Efficiency 2.3. Turbine Configuration 2.4. Part Load Operation Glossary Bibliography Biographical Sketch Summary The Carnot cycle is an ideal thermodynamic cycle based on the laws of thermodynamics. It indicates the maximum efficiency of a heat engine when operating between given temperatures of heat acceptance and heat rejection. The Rankine cycle is also an ideal cycle operating between two temperature limits but it is based on the principle of receiving heat by evaporation and rejecting heat by condensation. The working fluid is water-steam. In steam driven thermal power plants this basic cycle is modified by incorporating superheating and reheating to improve the performance of the turbine. UNESCO – EOLSS The Rankine cycle with its modifications suggests the best efficiency that can be obtained from this two phaseSAMPLE thermodynamic cycle wh enCHAPTERS operating under given temperature limits but its efficiency is less than that of the Carnot cycle since some heat is added at a lower temperature. The efficiency of the Rankine cycle can be improved by regenerative feedwater heating where some steam is taken from the turbine during the expansion process and used to preheat the feedwater before it is evaporated in the boiler. -
The Aircraft Propulsion the Aircraft Propulsion
THE AIRCRAFT PROPULSION Aircraft propulsion Contact: Ing. Miroslav Šplíchal, Ph.D. [email protected] Office: A1/0427 Aircraft propulsion Organization of the course Topics of the lectures: 1. History of AE, basic of thermodynamic of heat engines, 2-stroke and 4-stroke cycle 2. Basic parameters of piston engines, types of piston engines 3. Design of piston engines, crank mechanism, 4. Design of piston engines - auxiliary systems of piston engines, 5. Performance characteristics increase performance, propeller. 6. Turbine engines, introduction, input system, centrifugal compressor. 7. Turbine engines - axial compressor, combustion chamber. 8. Turbine engines – turbine, nozzles. 9. Turbine engines - increasing performance, construction of gas turbine engines, 10. Turbine engines - auxiliary systems, fuel-control system. 11. Turboprop engines, gearboxes, performance. 12. Maintenance of turbine engines 13. Ramjet engines and Rocket engines Aircraft propulsion Organization of the course Topics of the seminars: 1. Basic parameters of piston engine + presentation (1-7)- 3.10.2017 2. Parameters of centrifugal flow compressor + presentation(8-14) - 17.10.2017 3. Loading of turbine blade + presentation (15-21)- 31.10.2017 4. Jet engine cycle + presentation (22-28) - 14.11.2017 5. Presentation alternative date Seminar work: Aircraft engines presentation A short PowerPoint presentation, aprox. 10 minutes long. Content of presentation: - a brief history of the engine - the main innovation introduced by engine - engine drawing / cross-section - -
25 Kw Low-Temperature Stirling Engine for Heat Recovery, Solar, and Biomass Applications
25 kW Low-Temperature Stirling Engine for Heat Recovery, Solar, and Biomass Applications Lee SMITHa, Brian NUELa, Samuel P WEAVERa,*, Stefan BERKOWERa, Samuel C WEAVERb, Bill GROSSc aCool Energy, Inc, 5541 Central Avenue, Boulder CO 80301 bProton Power, Inc, 487 Sam Rayburn Parkway, Lenoir City TN 37771 cIdealab, 130 W. Union St, Pasadena CA 91103 *Corresponding author: [email protected] Keywords: Stirling engine, waste heat recovery, concentrating solar power, biomass power generation, low-temperature power generation, distributed generation ABSTRACT This paper covers the design, performance optimization, build, and test of a 25 kW Stirling engine that has demonstrated > 60% of the Carnot limit for thermal to electrical conversion efficiency at test conditions of 329 °C hot side temperature and 19 °C rejection temperature. These results were enabled by an engine design and construction that has minimal pressure drop in the gas flow path, thermal conduction losses that are limited by design, and which employs a novel rotary drive mechanism. Features of this engine design include high-surface- area heat exchangers, nitrogen as the working fluid, a single-acting alpha configuration, and a design target for operation between 150 °C and 400 °C. 1 1. INTRODUCTION Since 2006, Cool Energy, Inc. (CEI) has designed, fabricated, and tested five generations of low-temperature (150 °C to 400 °C) Stirling engines that drive internally integrated electric alternators. The fifth generation of engine built by Cool Energy is rated at 25 kW of electrical power output, and is trade-named the ThermoHeart® Engine. Sources of low-to-medium temperature thermal energy, such as internal combustion engine exhaust, industrial waste heat, flared gas, and small-scale solar heat, have relatively few methods available for conversion into more valuable electrical energy, and the thermal energy is usually wasted.