Chapter 19. Heat Engines and Refrigerators
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1 Chapter 19. Heat Engines and Refrigerators That s not smoke. It s clouds of water vapor rising from the cooling towers around a large power plant. The power plant is generating electricity by turning heat into work. Chapter Goal: To study the physical principles that govern the operation of heat engines and refrigerators.
2 Chapter 19. Heat Engines and Refrigerators Topics: Turning Heat into Work Heat Engines and Refrigerators Ideal-Gas Heat Engines Ideal-Gas Refrigerators The Limits of Efficiency The Carnot Cycle
3 Chapter 19. Reading Quizzes
4 What is the generic name for a cyclical device that transforms heat energy into work? A. Refrigerator B. Thermal motor C. Heat engine D. Carnot cycle E. Otto processor
5 What is the generic name for a cyclical device that transforms heat energy into work? A. Refrigerator B. Thermal motor C. Heat engine D. Carnot cycle E. Otto processor
6 The area enclosed within a pv curve is A. the work done by the system during one complete cycle. B. the work done on the system during one complete cycle. C. the thermal energy change of the system during one complete cycle. D. the heat transferred out of the system during one complete cycle.
7 The area enclosed within a pv curve is A. the work done by the system during one complete cycle. B. the work done on the system during one complete cycle. C. the thermal energy change of the system during one complete cycle. D. the heat transferred out of the system during one complete cycle.
8 The maximum possible efficiency of a heat engine is determined by A. its design. B. the amount of heat that flows. C. the maximum and minimum pressure. D. the compression ratio. E. the maximum and minimum temperature.
9 The maximum possible efficiency of a heat engine is determined by A. its design. B. the amount of heat that flows. C. the maximum and minimum pressure. D. the compression ratio. E. the maximum and minimum temperature.
10 The engine with the largest possible efficiency uses a A. Brayton cycle. B. Joule cycle. C. Carnot cycle. D. Otto cycle. E. Diesel cycle.
11 The engine with the largest possible efficiency uses a A. Brayton cycle. B. Joule cycle. C. Carnot cycle. D. Otto cycle. E. Diesel cycle.
12 Chapter 19. Basic Content and Examples
13 Turning Heat into Work Thermodynamics is the branch of physics that studies the transformation of energy. Many practical devices are designed to transform energy from one form, such as the heat from burning fuel, into another, such as work. Chapters 17 and 18 established two laws of thermodynamics that any such device must obey.
14 Heat Engines A heat engine is any closed-cycle device that extracts heat from a hot reservoir, does useful work, and exhausts heat to a cold reservoir. A closed-cycle device is one that periodically returns to its initial conditions, repeating the same process over and over. All state variables (pressure, temperature, thermal energy, and so on) return to their initial values once every cycle. A heat engine can continue to do useful work for as long as it is attached to the reservoirs.
15 Heat Engines
16 Heat Engines For practical reasons, we would like an engine to do the maximum amount of work with the minimum amount of fuel. We can measure the performance of a heat engine in terms of its thermal efficiency η (lowercase Greek eta), defined as We can also write the thermal efficiency as
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19 EXAMPLE 19.1 Analyzing a heat engine I QUESTION:
20 EXAMPLE 19.1 Analyzing a heat engine I
21 EXAMPLE 19.1 Analyzing a heat engine I
22 EXAMPLE 19.1 Analyzing a heat engine I
23 EXAMPLE 19.1 Analyzing a heat engine I
24 EXAMPLE 19.1 Analyzing a heat engine I
25 EXAMPLE 19.1 Analyzing a heat engine I
26 EXAMPLE 19.1 Analyzing a heat engine I
27 EXAMPLE 19.1 Analyzing a heat engine I
28 EXAMPLE 19.1 Analyzing a heat engine I
29 Problem-Solving Strategy: Heat-Engine Problems
30 Problem-Solving Strategy: Heat-Engine Problems
31 Problem-Solving Strategy: Heat-Engine Problems
32 Problem-Solving Strategy: Heat-Engine Problems
33 Problem-Solving Strategy: Heat-Engine Problems
34 Refrigerators Understanding a refrigerator is a little harder than understanding a heat engine. Heat is always transferred from a hotter object to a colder object. The gas in a refrigerator can extract heat Q C from the cold reservoir only if the gas temperature is lower than the cold-reservoir temperature T C. Heat energy is then transferred from the cold reservoir into the colder gas. The gas in a refrigerator can exhaust heat Q H to the hot reservoir only if the gas temperature is higher than the hot-reservoir temperature T H. Heat energy is then transferred from the warmer gas into the hot reservoir.
35 Refrigerators
36 Refrigerators
37 Refrigerators
38 EXAMPLE 19.3 Analyzing a refrigerator QUESTION:
39 EXAMPLE 19.3 Analyzing a refrigerator
40 EXAMPLE 19.3 Analyzing a refrigerator
41 EXAMPLE 19.3 Analyzing a refrigerator
42 EXAMPLE 19.3 Analyzing a refrigerator
43 EXAMPLE 19.3 Analyzing a refrigerator
44 EXAMPLE 19.3 Analyzing a refrigerator
45 EXAMPLE 19.3 Analyzing a refrigerator
46 The Limits of Efficiency Everyone knows that heat can produce motion. That it possesses vast motive power no one can doubt, in these days when the steam engine is everywhere so well known.... Notwithstanding the satisfactory condition to which they have been brought today, their theory is very little understood. The question has often been raised whether the motive power of heat is unbounded, or whether the possible improvements in steam engines have an assignable limit. Sadi Carnot
47 The Limits of Efficiency A perfectly reversible engine must use only two types of processes: 1. Frictionless mechanical interactions with no heat transfer (Q = 0) 2. Thermal interactions in which heat is transferred in an isothermal process ( E th = 0). Any engine that uses only these two types of processes is called a Carnot engine. A Carnot engine is a perfectly reversible engine; it has the maximum possible thermal efficiency η max and, if operated as a refrigerator, the maximum possible coefficient of performance K max.
48 The Carnot Cycle The Carnot cycle is an ideal-gas cycle that consists of the two adiabatic processes (Q = 0) and the two isothermal processes ( E th = 0) shown. These are the two types of processes allowed in a perfectly reversible gas engine.
49 The Carnot Cycle As a Carnot cycle operates, 1. The gas is isothermally compressed at T C. Heat energy Q C = Q 12 is removed. 2. The gas is adiabatically compressed, with Q = 0, until the gas temperature reaches T H. 3. After reaching maximum compression, the gas expands isothermally at temperature T H. Heat Q H = Q 34 is transferred into the gas. 4. The gas expands adiabatically, with Q = 0, until the temperature decreases back to T C. Work is done in all four processes of the Carnot cycle, but heat is transferred only during the two isothermal processes.
50 The Maximum Efficiency
51 EXAMPLE 19.6 Brayton versus Carnot
52 EXAMPLE 19.6 Brayton versus Carnot
53 EXAMPLE 19.6 Brayton versus Carnot
54 EXAMPLE 19.7 Generating electricity QUESTION:
55 EXAMPLE 19.7 Generating electricity
56 EXAMPLE 19.7 Generating electricity
57 EXAMPLE 19.7 Generating electricity
58 Chapter 19. Summary Slides
59 General Principles
60 General Principles
61 Important Concepts
62 Important Concepts
63 Important Concepts
64 Applications
65 Chapter 19. Questions
66 Rank in order, from largest to smallest, the work W out performed by these four heat engines. A. W b > W a > W c > W d B. W d > W a = W b > W c C. W b > W a > W b = W c D. W d > W a > W b > W c E. W b > W a > W b > W c
67 Rank in order, from largest to smallest, the work W out performed by these four heat engines. A. W b > W a > W c > W d B. W d > W a = W b > W c C. W b > W a > W b = W c D. W d > W a > W b > W c E. W b > W a > W b > W c
68 It s a really hot day and your air conditioner is broken. Your roommate says, Let s open the refrigerator door and cool this place off. Will this work? A. Yes. B. No. C. It might, but it will depend on how hot the room is.
69 It s a really hot day and your air conditioner is broken. Your roommate says, Let s open the refrigerator door and cool this place off. Will this work? A. Yes. B. No. C. It might, but it will depend on how hot the room is.
70 What is the thermal efficiency of this heat engine? A. 4 B C D E. Can t tell without knowing Q C.
71 What is the thermal efficiency of this heat engine? A. 4 B C D E. Can t tell without knowing Q C.
72 What, if anything, is wrong with this refrigerator? A. It violates the second law of thermodynamics. B. It violates the third law of thermodynamics. C. It violates the first law of thermodynamics. D. Nothing is wrong.
73 What, if anything, is wrong with this refrigerator? A. It violates the second law of thermodynamics. B. It violates the third law of thermodynamics. C. It violates the first law of thermodynamics. D. Nothing is wrong.
74 Could this heat engine be built? A. No. B. Yes. C. It s impossible to tell without knowing what kind of cycle it uses.
75 Could this heat engine be built? A. No. B. Yes. C. It s impossible to tell without knowing what kind of cycle it uses.
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