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Thermodynamics
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1-14 Chapter Summary The first law of thermodynamics is simply an expression of the conservation of energy principle, and it asserts that energy is a thermodynamic property. The second law of thermodynamics asserts that energy has quality as well as quantity, and actual processes occur in the direction of decreasing quality of energy.
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1-15 Chapter Summary A system of fixed mass is called a closed system, or control mass, and a system that involves mass transfer across its boundaries is called an open system, or control volume.
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1-16 Chapter Summary The mass-dependent properties of a system are called extensive properties and the others, intensive properties. Density is mass per unit volume, and specific volume is volume per unit mass.
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1-17 Chapter Summary The sum of all forms of energy of a system is called total energy, which is considered to consist of internal, kinetic, and potential energies. Internal energy represents the molecular energy of a system and may exist in sensible, latent, chemical, and nuclear forms.
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1-18 Chapter Summary A system is said to be in thermodynamic equilibrium if it maintains thermal, mechanical, phase, and chemical equilibrium.
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1-19 Chapter Summary Any change from one state to another is called a process. A process with identical end states is called a cycle.
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1-20 Chapter Summary During a quasi-static or quasi-equilibrium process, the system remains practically in equilibrium at all times.
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1-21 Chapter Summary The state of a simple, compressible system is completely specified by two independent, intensive properties.
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1-22 Chapter Summary Force per unit area is called pressure, and its unit is the pascal. The absolute, gage, and vacuum pressures are related by
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1-23 Chapter Summary Small to moderate pressure differences are measured by a manometer, and a differential fluid column of height h corresponds to a pressure difference of where is the fluid density and g is the local gravitational acceleration.
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1-24 Chapter Summary The atmospheric pressure is measured by a barometer and is determined from where h is the height of the liquid column above the free surface.
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1-25 Chapter Summary The zeroth law of thermodynamics states that two bodies are in thermal equilibrium if both have the same temperature reading even if they are not in contact.
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1-26 Chapter Summary The temperature scales used in the SI and the English system today are the Celsius scale and the Fahrenheit scale, respectively.
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1-27 Chapter Summary The absolute temperature scale in the SI is the Kelvin scale, which is related to the Celsius scale by
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1-28 Chapter Summary In the English system, the absolute temperature scale is the Rankine scale, which is related to the Fahrenheit scale by
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1-29 Chapter Summary The magnitudes of each division of 1 K and 1 0C are identical, and so are the magnitude of each division of 1 R and 10F. Therefore, and
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1-30 Chapter Summary An important application area of thermodynamics is the biological system. Most diets are based on the simple energy balance: the net energy gained by a person in the form of fat is equal to the difference between the energy intake from food and the energy expended by exercise.
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1 CHAPTER Basic Concepts of Thermodynamics
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Applications of Thermodynamics
1-1 Applications of Thermodynamics Power plants The human body Air-conditioning systems Airplanes Car radiators Refrigeration systems
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Crossing Closed-System Boundries
1-2 Crossing Closed-System Boundries Energy, not mass, crosses closed-system boundries (Fig. 1-13)
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Closed System with Moving Boundry
1-3 Closed System with Moving Boundry
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Crossing Control Volume Boundaries
1-4 Crossing Control Volume Boundaries Mass and Energy Cross Control Volume Boundaries
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System’s Internal Energy
1-5 System’s Internal Energy System’s Internal Energy = Sum of Microscopic Energies (Fig. 1-19)
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Quasi-Equilibrium, Work-Producing Devices
1-6 Quasi-Equilibrium, Work-Producing Devices Quasi-Equilibrium, Work-Producing Devices Deliver the Most Work (Fig. 1-30)
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Compressed Process P-V Diagram
1-7 Compressed Process P-V Diagram (Fig. 1-31)
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Absolute, Gage, and Vacuum Pressures
1-8 Absolute, Gage, and Vacuum Pressures (Fig. 1-36)
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1-9 The Basic Manometer
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Temperature Scales Comparison
1-10 Temperature Scales Comparison (Fig. 1-48)
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Many Ways to Supply the Same Energy
1-11 Many Ways to Supply the Same Energy Ways to supply a room with energy equalling a 300-W electric resistance heater (Fig. 1-52)
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Bomb Calorimeter Used to Determine Energy Content of Food
1-12 Bomb Calorimeter Used to Determine Energy Content of Food (Fig. 1-53)
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1-13 Chapter Summary Thermodynamics is the science that primarily deals with energy.
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1-14 Chapter Summary The first law of thermodynamics is simply an expression of the conservation of energy principle, and it asserts that energy is a thermodynamic property. The second law of thermodynamics asserts that energy has quality as well as quantity, and actual processes occur in the direction of decreasing quality of energy.
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1-15 Chapter Summary A system of fixed mass is called a closed system, or control mass, and a system that involves mass transfer across its boundaries is called an open system, or control volume.
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1-16 Chapter Summary The mass-dependent properties of a system are called extensive properties and the others, intensive properties. Density is mass per unit volume, and specific volume is volume per unit mass.
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1-17 Chapter Summary The sum of all forms of energy of a system is called total energy, which is considered to consist of internal, kinetic, and potential energies. Internal energy represents the molecular energy of a system and may exist in sensible, latent, chemical, and nuclear forms.
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1-18 Chapter Summary A system is said to be in thermodynamic equilibrium if it maintains thermal, mechanical, phase, and chemical equilibrium.
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1-19 Chapter Summary Any change from one state to another is called a process. A process with identical end states is called a cycle.
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1-20 Chapter Summary During a quasi-static or quasi-equilibrium process, the system remains practically in equilibrium at all times.
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1-21 Chapter Summary The state of a simple, compressible system is completely specified by two independent, intensive properties.
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1-22 Chapter Summary Force per unit area is called pressure, and its unit is the pascal. The absolute, gage, and vacuum pressures are related by
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1-23 Chapter Summary Small to moderate pressure differences are measured by a manometer, and a differential fluid column of height h corresponds to a pressure difference of where is the fluid density and g is the local gravitational acceleration.
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1-24 Chapter Summary The atmospheric pressure is measured by a barometer and is determined from where h is the height of the liquid column above the free surface.
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1-25 Chapter Summary The zeroth law of thermodynamics states that two bodies are in thermal equilibrium if both have the same temperature reading even if they are not in contact.
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1-26 Chapter Summary The temperature scales used in the SI and the English system today are the Celsius scale and the Fahrenheit scale, respectively.
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1-27 Chapter Summary The absolute temperature scale in the SI is the Kelvin scale, which is related to the Celsius scale by
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1-28 Chapter Summary In the English system, the absolute temperature scale is the Rankine scale, which is related to the Fahrenheit scale by
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1-29 Chapter Summary The magnitudes of each division of 1 K and 1 0C are identical, and so are the magnitude of each division of 1 R and 10F. Therefore, and
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1-30 Chapter Summary An important application area of thermodynamics is the biological system. Most diets are based on the simple energy balance: the net energy gained by a person in the form of fat is equal to the difference between the energy intake from food and the energy expended by exercise.
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