Chapter 22 - 22 CHAPTER OUTLINE 22.1 Heat Engines and the...

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Unformatted text preview: 22 CHAPTER OUTLINE 22.1 Heat Engines and the Second Law of Thermodynamics 22.2 Heat Pumps and Refrigerators 22.3 Reversible and Irreversible Processes 22.4 The Carnot Engine 22.5 Gasoline and Diesel Engines 22.6 Entropy 22.7 Entropy Changes in Irreversible Processes Scale 22.8 Entropy on a Microscopic Heat Engines, Entropy, and the Second Law of Thermodynamics ANSWERS TO QUESTIONS Q22.1 First, the efficiency of the automobile engine cannot exceed the Carnot efficiency: it is limited by the temperature of burning fuel and the temperature of the environment into which the exhaust is dumped. Second, the engine block cannot be allowed to go over a certain temperature. Third, any practical engine has friction, incomplete burning of fuel, and limits set by timing and energy transfer by heat. Q22.2 It is easier to control the temperature of a hot reservoir. If it cools down, then heat can be added through some external means, like an exothermic reaction. If it gets too hot, then heat can be allowed to “escape” into the atmosphere. To maintain the temperature of a cold reservoir, one must remove heat if the reservoir gets too hot. Doing this requires either an “even colder” reservoir, which you also must maintain, or an endothermic process. Q22.3 A higher steam temperature means that more energy can be extracted from the steam. For a constant temperature heat sink at T c , and steam at T h , the efficiency of the power plant goes as T T T T T h c h c h − = − 1 and is maximized for a high T h . Q22.4 No. Any heat engine takes in energy by heat and must also put out energy by heat. The energy that is dumped as exhaust into the low-temperature sink will always be thermal pollution in the outside environment. So-called ‘steady growth’ in human energy use cannot continue. Q22.5 No. The first law of thermodynamics is a statement about energy conservation, while the second is a statement about stable thermal equilibrium. They are by no means mutually exclusive. For the particular case of a cycling heat engine, the first law implies Q W Q h e n g c = + , and the second law implies Q c > 0. Q22.6 Take an automobile as an example. According to the first law or the idea of energy conservation, it must take in all the energy it puts out. Its energy source is chemical energy in gasoline. During the combustion process, some of that energy goes into moving the pistons and eventually into the mechanical motion of the car. Clearly much of the energy goes into heat, which, through the cooling system, is dissipated into the atmosphere. Moreover, there are numerous places where friction, both mechanical and fluid, turns mechanical energy into heat. In even the most efficient internal combustion engine cars, less than 30% of the energy from the fuel actually goes into moving the car....
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Chapter 22 - 22 CHAPTER OUTLINE 22.1 Heat Engines and the...

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