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Temperature, Heat, and the First Law of Thermodynamics
Chapter 18 Temperature, Heat, and the First Law of Thermodynamics
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Temperature Thermodynamics – branch of physics studying thermal energy of systems Temperature (T), a scalar – measure of the thermal (internal) energy of a system SI unit: K (Kelvin) Kelvin scale has a lower limit (absolute zero) and has no upper limit William Thomson (Lord Kelvin) ( )
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Kelvin scale Kelvin scale is defined by the temperature of the triple point of pure water Triple point – set of pressure and temperature values at which solid, liquid, and gas phases can coexist International convention: T of the triple point of water is
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The zeroth law of thermodynamics
If two (or more) bodies in contact don’t change their internal energy with time, they are in thermal equilibrium 0th law of thermodynamics: if bodies are in thermal equilibrium, their temperatures are equal
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Measuring temperature
Temperature measurement principle: if bodies A and B are each in thermal equilibrium with a third body T, then A and B are in thermal equilibrium with each other (and their temperatures are equal) The standard temperature for the Kelvin scale is measured by the constant-volume gas thermometer
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Constant-volume gas thermometer
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Celsius and Fahrenheit scales
Celsius scale: Fahrenheit scale: Anders Cornelius Celsius ( ) Gabriel Daniel Fahrenheit ( )
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Thermal expansion Thermal expansion: increase in size with an increase of a temperature Linear expansion: Volume expansion:
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Chapter 18 Problem 19
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Temperature and heat Heat (Q): energy transferred between a system and its environment because of a temperature difference that exists between them SI Unit: Joule Alternative unit: calorie (cal):
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Q Q Absorption of heat Specific heat (c): heat capacity per unit mass
Common states (phases) of matter: solid, liquid, gas Heat of transformation (L): the amount of energy per unit mass transferred during a phase change (boiling, condensation, melting, freezing, etc.) Q Q
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Chapter 18 Problem 37
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Heat and work Thermodynamic cycle
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The first law of thermodynamics
Work and heat are path-dependent quantities Quantity Q – W = Eint (internal energy) is path-independent 1st law of thermodynamics: the internal energy of a system increases if heat is added to the system and decreases if work is done by the system
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The first law of thermodynamics
Adiabatic process: no heat transfer between the system and the environment Isochoric (constant volume) process Free expansion: Cyclical process:
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Chapter 18 Problem 48
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Heat transfer mechanisms
Thermal conduction Conduction rate: Thermal resistance: Conduction through a composite slab: Thermal conductivity
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Heat transfer mechanisms
Thermal radiation Radiation rate: Stefan-Boltzmann constant: Absorption rate: Emissivity Josef Stefan ( ) Ludwig Eduard Boltzmann ( )
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Chapter 18 Problem 52
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Heat transfer mechanisms
Convection
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Heat transfer mechanisms
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Answers to the even-numbered problems
Chapter 18: Problem 4 320º F; (b) -12.3º F
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Answers to the even-numbered problems
Chapter 18: Problem 10 1.1 cm
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Answers to the even-numbered problems
Chapter 18: Problem 22 109 g
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Answers to the even-numbered problems
Chapter 18: Problem 44 − 200 J; (b) − 293 J; (c) − 93 J
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Answers to the even-numbered problems
Chapter 18: Problem 50 0.42 m; (b) 7.4 km
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