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Chapter 23 The First Law of Thermodynamics
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Thermal Physics Macroscopic Microscopic The Diffusion The Viscous The Transfer of Heat Exchange molecule T A A T B B Q
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The Transfer of Heat T A < T B Thermal Conducting T A A T B B Q
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Work done on a system by external forces System K, U Mechanical Energy The first law of thermodynamics state functions as T, p, V heat and work notprocess
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The first law of thermodynamics Process Initial State Final State
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The first law of thermodynamics Process Initial State Final State
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Heat Capacity Specific Heat
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T Q added to water water temp rises water changes to steam (boils) steam temp rises 100 o C Pressure keeps at 1 atm Latent Heat Heat needed to add to or remove from a substance to change the state of it: The Ideal Gas
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Kinetic energy
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Monatomic Molecule
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Diatomic Molecule Equipartition of Energy Theorem: When the number of molecules is large, the average energy per molecule is kT/2 for each independent degree of freedom.
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After Collision Reducing Translation Motion Increasing Rotational Motion
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After Collision Reducing Rotational Motion Increasing Translation Motion Finally Rotational Motion = Translation Motion
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polyatomic Molecule
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Molecule in Solid
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polyatomic Molecule Diatomic Molecule Monatomic Molecule
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Molar Heat Capacity of Solid Molar Heat Capacity T Aluminum Lead 0
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Ideal Gas
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Constant Volume
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Ideal Gas Constant Volume
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Ideal Gas Constant temperature
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Example
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Polyatomic Molecule Diatomic Molecule Monatomic Molecule The Internal Energy of an Ideal Gas
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Constant Volume The Molar Heat Capacity of an Ideal Gas Monatomic Molecule Diatomic MoleculePolyatomic Molecule
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Constant Pressure The Molar Heat Capacity of an Ideal Gas Monatomic Molecule Diatomic Molecule
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Constant Pressure The Molar Heat Capacity of an Ideal Gas Monatomic MoleculeDiatomic Molecule Polyatomic Molecule
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CHAP. 23 Exercises P540 11, 19, 21 P541 24, 25
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The Molar Heat Capacity of an Ideal Gas Monatomic Molecule Diatomic Molecule Polyatomic Molecule
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The Molar Heat Capacity of an Ideal Gas R: molar gas constant
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Work Done in adiabatic process
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Adiabatic process Constant temperature
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p reduces quickly in thermal Isolation The first law of thermodynamics p is lower in thermal Isolation Adiabatic process Constant temperature Thermal Isolation (adiabatic process)
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The first law of thermodynamics Process Initial State Final State The Ideal Gas
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Constant Volume Process Constant Pressure Process Constant Temperatu re Process adiabatic process Constant Volume Constant Pressure
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a b p p/2 V/2 V
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Cyclical process
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Heat Engine
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Thermal Efficiency
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Example Thermal Efficiency?
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Example Thermal Efficiency?
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Example Thermal Efficiency?
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Example Constant Temperature Thermal Isolation Constant Temperature Thermal Isolation Thermal Efficiency? The Carnot Cycle The Carnot Engine
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Q2Q2 W Q1Q1 T1T1 T2T2 Refrigerator Q2Q2 W T2T2 Q1Q1 T1T1
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Q2Q2 W T2T2 Q1Q1 T1T1 TXTX Q TXTX Q
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Q T1T1 T2T2 Q T1T1 T2T2 Irreversible Process Q2Q2 W T2T2 Q1Q1 T1T1
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Work Done in Thermal Isolation Change of the state Free Expansion Nonequilibrium Process reversible Irreversible
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The first law of thermodynamics Process Initial State Final State reversibleIrreversible The second law of thermodynamics
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CHAP.23 Exercises P542 40, 45, 46 CHAP.24 Exercises P564 21, 22
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