Atkinson cycle From Wikipedia, the free encyclopedia Jump to: navigation, search Thermodynamics Branches Classical · Statistical · Chemical Equilibrium / Non-equilibrium Thermofluids Laws Zeroth · First · Second · Third Systems State: Equation of state Ideal gas · Real gas Phase of matter · Equilibrium Control volume · Instruments Processes: Isobaric · Isochoric · Isothermal Adiabatic · Isentropic · Isenthalpic Quasistatic · Polytropic Free expansion Reversibility · Irreversibility Endoreversibility Cycles: Heat engines · Heat pumps Thermal efficiency System properties Property diagrams Intensive and extensive properties State functions: Temperature / Entropy (intro.) † Pressure / Volume † Chemical potential / Particle no. † († Conjugate variables) Vapor quality Reduced properties Process functions: Work · Heat Material properties Specific heat c= capacity Compressibility T N β= 1 − V Thermal expansion α = 1 V Property database Equations Carnot's theorem Clausius theorem Fundamental relation Ideal gas law Maxwell relations Table of thermodynamic equations Potentials Free energy · Free entropy Internal energy U(S,V) H(S,p) Enthalpy = U +pV Helmholtz free A(T,V) energy = U −TS G(T,p) Gibbs free energy = H −TS History and culture Philosophy: Entropy and time · Entropy and life Brownian ratchet Maxwell's demon Heat death paradox Loschmidt's paradox Synergetics History: General · Heat · Entropy · Gas laws Perpetual motion Theories: Caloric theory · Vis viva Theory of heat Mechanical equivalent of heat Motive power Publications: "An Experimental Enquiry Concerning ... Heat" "On the Equilibrium of Heterogeneous Substances" "Reflections on the Motive Power of Fire" Timelines of: Thermodynamics · Heat engines Art: Maxwell's thermodynamic surface Education: Entropy as energy dispersal Scientists Daniel Bernoulli Sadi Carnot Benoît Paul Émile Clapeyron Rudolf Clausius Hermann von Helmholtz Constantin Carathéodory James Prescott Joule Julius Robert von Mayer William Rankine John Smeaton Georg Ernst Stahl Benjamin Thompson William Thomson, 1st Baron Kelvin John James Waterston v·d·e The Atkinson cycle engine is a type of internal combustion engine invented by James Atkinson in 1882. The Atkinson cycle is designed to provide efficiency at the expense of power density, and is used in some modern hybrid electric applications. Contents 1 Design 2 Ideal thermodynamic cycle 3 Modern Atkinson cycle engines 4 Rotary Atkinson cycle engine 5 Vehicles using Atkinson cycle engines 6 See also 7 References 8 External links [edit] Design The original Atkinson cycle piston engine allowed the intake, compression, power, and exhaust strokes of the four-stroke cycle to occur in a single turn of the crankshaft and was designed to avoid infringing certain patents covering Otto cycle engines.[1] Because of the unique crankshaft design of the Atkinson, its expansion ratio can differ from its compression ratio and, with a power stroke longer than its compression stroke, the engine can achieve greater thermal efficiency than a traditional piston engine. While Atkinson's original design is no more than an historical curiosity, many modern engines use unconventional valve timing to produce the effect of a shorter compression stroke/longer power stroke, thus realizing the fuel economy improvements the Atkinson cycle can provide.[2] [edit] Ideal thermodynamic cycle Figure 1: Atkinson Gas Cycle The ideal Atkinson cycle consists of following operations: 1-2 Isentropic or reversible adiabatic compression 2-3 Isochoric heating (Qp) 3-4 Isobaric heating (Qp') 4-5 Isentropic expansion 5-6 Isochoric cooling (Qo) 6-1 Isobaric cooling (Qo') [edit] Modern Atkinson cycle engines A small engine with Atkinson-style linkages between the piston and flywheel. Modern Atkinson cycle engines do away with this complex energy path. Recently Atkinson cycle has been used to describe a modified Otto cycle engine in which the intake valve is held open longer than normal to allow a reverse flow of intake air into the intake manifold. The effective compression ratio is reduced (for a time the air is escaping the cylinder freely rather than being compressed) but the expansion ratio is unchanged. This means the compression ratio is smaller than the expansion ratio. Heat gained from burning fuel increases the pressure, thereby forcing the piston to move, expanding the air volume beyond the volume when compression began. The goal of the modern Atkinson cycle is to allow the pressure in the combustion chamber at the end of the power stroke to be equal to atmospheric pressure; when this occurs, all the available energy has been obtained from the combustion process. For any given portion of air, the greater expansion ratio allows more energy to be converted from heat to useful mechanical energy meaning the engine is more efficient. The disadvantage of the four-stroke Atkinson cycle engine versus the more common Otto cycle engine is reduced power density. Because a smaller portion of the compression stroke is devoted to compressing the intake air, an Atkinson cycle engine does not take in as much air as would a similarly designed and sized Otto cycle engine. Four-stroke engines of this type with this same type of intake valve motion but with a supercharger to make up for the loss of power density are known as Miller cycle engines. [edit] Rotary Atkinson cycle engine Rotary Atkinson cycle engine The Atkinson cycle can be used in a rotary engine. In this configuration an increase in both power and efficiency can be achieved when compared to the Otto cycle. This type of engine retains the one power phase per revolution, together with the different compression and expansion volumes of the original Atkinson cycle. Exhaust gases are expelled from the engine by compressed-air scavenging. This modification of the Atkinson cycle allows for the use of alternative fuels like diesel and hydrogen. Disadvantages of this design include the requirement that rotor tips seal very tightly on the outer housing wall and the mechanical losses suffered through friction between rapidly oscillating parts of irregular shape. See External Links for more information. [edit] Vehicles using Atkinson cycle engines 2004 Toyota Prius hybrid 2009 Ford Fusion Hybrid, as sold in the United States. Unrelated to the European car of the same name. While a modified Otto cycle engine using the Atkinson cycle provides good fuel economy, it is at the expense of a lower power-per-displacement as compared to a traditional four-stroke engine.[3] If demand for more power is intermittent, the power of the engine can be supplemented by an electric motor during times when more power is needed. This forms the basis of an Atkinson cycle-based hybrid electric drivetrain. These electric motors can be used independently of, or in combination with, the Atkinson cycle engine, to provide the most efficient means of producing the desired power. Several production vehicles use Atkinson cycle engines: Chevrolet Tahoe Hybrid hybrid electric (four-wheel drive) with a compression ratio of 10.8:1 Ford Escape/Mercury Mariner/Mazda Tribute hybrid electric (front- and fourwheel drive) with a compression ratio of 12.4:1 Ford Fusion Hybrid/Mercury Milan Hybrid/Lincoln MKZ Hybrid hybrid electric (front-wheel drive) with a compression ratio of 12.3:1 Hyundai Sonata Hybrid (front-wheel drive) Infiniti M35h Hybrid (rear-wheel drive) Kia Optima Hybrid (front-wheel drive) Lexus CT200H (front-wheel drive) Lexus HS250h (front-wheel drive) Lexus RX 450h hybrid electric (front-wheel drive) Mercedes ML450 Hybrid (four-wheel drive) hybrid electric Mercedes S400 Blue Hybrid (rear-wheel drive) hybrid electric Toyota Prius hybrid electric (front-wheel drive) with a (purely geometric) compression ratio of 13.0:1 Toyota Camry Hybrid hybrid electric (front-wheel drive) with a compression ratio of 12.5:1 Note that the compression ratios shown above reflect the expansion ratio, which is the ratio of the combustion chamber volumes when the piston is at bottom dead centre and top dead centre. The effective compression ratio of the air-fuel mixture in an Atkinson cycle engine, with respect to atmospheric pressure, is lower due to the aforementioned delay in closing the intake valve [edit] See also History of the internal combustion engine [edit] References 1. ^ U.S. Patent 367,496 2. ^ http://www.canadiandriver.com/2010/07/14/auto-tech-atkinson-cycleengines-and-hybrids.htm 3. ^ Heywood, John B. Internal Combustion Engine Fundamentals, pp. 184-186.