(BQ) Part 2 book Thermodynamics has contents: Gas power cycles, vapor and combined power cycles, refrigeration cycles; thermodynamic property relations, gas mixtures, gas mixtures, chemical reactions, chemical and phase equilibrium, chemical and phase equilibrium,... and other contents.
CHAPTER GAS P O W E R C Y C L E S wo important areas of application for thermodynamics are power generation and refrigeration Both are usually accomplished by sys tems that operate on a thermodynamic cycle Thermodynamic cycles can be divided into two general categories: power cycles, which are dis cussed in this chapter and Chap 10, and refrigeration cycles, which are discussed in Chap 11 The devices or systems used to produce a net power output are often called engines, and the thermodynamic cycles they operate on are called pow er cycles The devices or systems used to produce a refrigeration effect are called refrigerators, air conditioners, or heat pumps, and the cycles they operate on are called refrigeration cycles Thermodynamic cycles can also be categorized as gas cycles and vapor cycles, depending on the phase of the working fluid In gas cycles, the working fluid remains in the gaseous phase throughout the entire cycle, whereas in vapor cycles the working fluid exists in the vapor phase during one part of the cycle and in the liquid phase during another part Thermodynamic cycles can be categorized yet another way: closed and open cycles In closed cycles, the working fluid is returned to the initial state at the end of the cycle and is recirculated In open cycles, the working fluid is renewed at the end of each cycle instead of being recirculated In automobile engines, the combustion gases are exhausted and replaced by fresh air-fuel mixture at the end of each cycle The engine operates on a mechanical cycle, but the working fluid does not go through a complete thermodynamic cycle Heat engines are categorized as internal combustion and external combus tion engines, depending on how the heat is supplied to the working fluid In external combustion engines (such as steam power plants), heat is supplied to the working fluid from an external source such as a furnace, a geothermal well, a nuclear reactor, or even the sun In internal combustion engines (such as automobile engines), this is done by burning the fuel within the system boundaries In this chapter, various gas power cycles are analyzed under some simplifying assumptions T CgO:f Objectives The objectives of Chapter are to: ■ Evaluate the performance of gas power cycles for which the working fluid remains a gas throughout the entire cycle ■ Develop sim plifying assumptions applicable to gas power cycles i Review the operation of reciprocating engines i Analyze both closed and open gas power cycles Solve problems based on the Otto, Diesel, Stirling, and Ericsson cycles Solve problems based on the Brayton cycle; the Brayton cycle with regeneration; and the Brayton cycle w ith intercooling, reheating, and regeneration Analyze jet-propulsion cycles Identify sim plifying assumptions for second-law analysis of gas power cycles Perform second-law analysis of gas power cycles 488 GAS POWER CYCLES j 9-1 - BASIC CONSIDERATIONS IN THE ANALYSIS OF POWER CYCLES Oven A Id eal \ W ater A ctual 175°C I P o ta to , FIGURE 9-1 Modeling is a powerful engineering tool that provides great insight and simplicity at the expense of some loss in accuracy FIGURE -2 The analysis of many complex processes can be reduced to a manageable level by utilizing some idealizations Most power-producing devices operate on cycles, and the study of power cycles is an exciting and important part of thermodynamics The cycles encountered in actual devices are difficult to analyze because of the pres ence of complicating effects, such as friction, and the absence of sufficient time for establishment of the equilibrium conditions during the cycle To make an analytical study of a cycle feasible, we have to keep the complexi ties at a manageable level and utilize some idealizations (Fig 9-1) When the actual cycle is stripped of all the internal irreversibilities and complexities, we end up with a cycle that resembles the actual cycle closely but is made up totally of internally reversible processes Such a cycle is called an ideal cycle (Fig 9-2) A simple idealized model enables engineers to study the effects of the major parameters that dominate the cycle without getting bogged down in the details The cycles discussed in this chapter are somewhat idealized, but they still retain the general characteristics of the actual cycles they repre sent The conclusions reached from the analysis of ideal cycles are also applicable to actual cycles The thermal efficiency of the Otto cycle, the ideal cycle for spark-ignition automobile engines, for example, increases with the compression ratio This is also the case for actual automobile engines The numerical values obtained from the analysis of an ideal cycle, however, are not necessarily representative of the actual cycles, and care should be exercised in their interpretation (Fig 9-3) The simplified analy sis presented in this chapter for various power cycles of practical interest may also serve as the starting point for a more in-depth study Heat engines are designed for the purpose of converting thermal energy to work, and their performance is expressed in terms of the thermal efficiency 7jth, which is the ratio of the net work produced by the engine to the total heat input: ^net hm m m / i f y o u o u t OFF THE Vth = r~ in or w net 17th = — (9-1) T in LEGS OF A F L E A IT BECOMES D E A F.' FIGURE -3 Care should be exercised in the interpretation of the results from ideal cycles B LO N D IE © K ING FE ATU RES SYNDICATE Recall that heat engines that operate on a totally reversible cycle, such as the Carnot cycle, have the highest thermal efficiency of all heat engines operating between the same temperature levels That is, nobody can develop a cycle more efficient than the C am ot cycle Then the following question arises naturally: If the Carnot cycle is the best possible cycle, why we not use it as the model cycle for all the heat engines instead of bothering with several so-called ideal cycles? The answer to this question is hardwarerelated Most cycles encountered in practice differ significantly from the Carnot cycle, which makes it unsuitable as a realistic model Each ideal cycle discussed in this chapter is related to a specific work-producing device and is an idealized version of the actual cycle The ideal cycles are internally reversible, but, unlike the Camot cycle, they are not necessarily externally reversible That is, they may involve irreversibil ities external to the system such as heat transfer through a finite temperature difference Therefore, the thermal efficiency of an ideal cycle, in general, is less than that of a totally reversible cycle operating between the same FIGURE -4 An automotive engine with the combustion chamber exposed Courtesy o f General Motors temperature limits However, it is still considerably higher than the thermal efficiency of an actual cycle because of the idealizations utilized (Fig 9—4) The idealizations and simplifications commonly employed in the analysis of power cycles can be summarized as follows: The cycle does not involve any friction Therefore, the working fluid does not experience any pressure drop as it flows in pipes or devices such as heat exchangers All expansion and compression processes take place in a quasi equilibrium manner The pipes connecting the various components of a system are well insulated, and heat transfer through them is negligible Neglecting the changes in kinetic and potential energies of the working fluid is another commonly utilized simplification in the analysis of power cycles This is a reasonable assumption since in devices that involve shaft work, such as turbines, compressors, and pumps, the kinetic and potential energy terms are usually very small relative to the other terms in the energy equation Fluid velocities encountered in devices such as condensers, boil ers, and mixing chambers are typically low, and the fluid streams experience little change in their velocities, again making kinetic energy changes negli gible The only devices where the changes in kinetic energy are significant are the nozzles and diffusers, which are specifically designed to create large changes in velocity In the preceding chapters, property diagrams such as the P-w and T-s dia grams have served as valuable aids in the analysis of thermodynamic processes On both the P-w and T-s diagrams, the area enclosed by the process curves of a cycle represents the net work produced during the cycle (Fig 9-5), which is also equivalent to the net heat transfer for that cycle The T-s diagram is particularly useful as a visual aid in the analysis of ideal PI s FIGURE -5 On both P-v and T-s diagrams, the area enclosed by the process curve represents the net work of the cycle 490 GAS POWER CYCLES power cycles An ideal power cycle does not involve any internal irre versibilities, and so the only effect that can change the entropy of the work ing fluid during a process is heat transfer On a T-s diagram, a heat-addition process proceeds in the direction of increasing entropy, a heat-rejection process proceeds in the direction of decreasing entropy, and an isentropic (internally reversible, adiabatic) process proceeds at constant entropy The area under the process curve on a T-s diagram represents the heat transfer for that process The area under the heat addition process on a T-s diagram is a geometric measure of the total heat supplied during the cycle qm, and the area under the heat rejection process is a measure of the total heat rejected qnM The difference between these two (the area enclosed by the cyclic curve) is the net heat transfer, which is also the net work produced during the cycle Therefore, on a T-s diagram, the ratio of the area enclosed by the cyclic curve to the area under the heat-addition process curve represents the thermal efficiency of the cycle Any modification that increases the ratio o f these two areas will also increase the thermal efficiency o f the cycle Although the working fluid in an ideal power cycle operates on a closed loop, the type of individual processes that comprises the cycle depends on the individual devices used to execute the cycle In the Rankine cycle, which is the ideal cycle for steam power plants, the working fluid flows through a series of steady-flow devices such as the turbine and condenser, whereas in the Otto cycle, which is the ideal cycle for the spark-ignition automobile engine, the working fluid is alternately expanded and compressed in a pistoncylinder device Therefore, equations pertaining to steady-flow systems should be used in the analysis of the Rankine cycle, and equations pertaining to closed systems should be used in the analysis of the Otto cycle k o CX 'cl C a)