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Temperature Physics 313 Professor Lee Carkner Lecture 2
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Thermodynamics Thermodynamics is the study of energy e.g. a cylinder of gas accelerated to high speed has an increased kinetic energy but the same temperature We will discuss the properties of a system and how they relate to internal energy, through both the macroscopic and microscopic points of view
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Macroscopic Microscopic Specify a few basic bulk properties Classical Thermodynamics Specify states of individual units Statistical mechanics
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Systems Material separated from its surroundings by a boundary Closed e.g. gas in a piston Open e.g. an automobile radiator
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Processes State Process Quasi - Static (Quasi-Equilibrium) Process slow changes Non-quasi static processes are discontinuous
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Equilibrium Define two properties for a system If the two properties remain constant the system is in equilibrium A system is in equilibrium with itself if its properties are constant throughout the whole system
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System Boundaries Adiabatic Wall thermal insulator Dithermal wall thermal conductor
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Temperature Proxies Changes in temperature cause changes in other system properties Two consequences: We measure T by measuring changes in other properties If T is not constant, nothing else is Often given at standard temperature (0 C) or room temperature (20 C)
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Thermal Expansion The degree to which a linear distance varies with temperature is given by: Change in one dimension (linear expansion) Very small (~one part in a million per degree) in most cases Note that itself is temperature dependant
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Typical “toothed” bridge expansion joint
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“Rocker” support that allows deck expansion
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“Sleeved” railing expansion section
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The Brooklyn Bridge
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Built: Designed: John A Roebling Chief Engineer: Washington A. Roebling Height: Length: World’s longest suspension bridge until 1903 To learn more about the Brooklyn Bridge visit your local library: The Great Bridge : The Epic Story of the Building of the Brooklyn Bridge by David McCullough
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Brooklyn Bridge cables
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Stringing the Cables
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Main Cable
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Thermal Equilibrium Two systems separated by a dithermal wall that do not change properties If the two systems are not in thermal equilibrium they will exchange heat until they are
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Zeroth Law Three systems A, B and T A and T -- B and T -- Then for A and B Two systems in thermal equilibrium with a third are in thermal equilibrium with each other
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Isotherms Plot pressure and volume Curve is called an isotherm Temperature determines thermal equilibrium
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Temperature Take an object T and mark it so that changes in its properties can be measured Calibrate the measurements so that your scale corresponds to universally accepted situations e.g. mercury thermometer
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Temperature Scales Gabriel Daniel Fahrenheit invented the mercury thermometer in 1714 32 F is freezing point of water, 212 is chosen for boiling point (32+180) Anders Celsius introduced his scale in 1742 William Thomson, Lord Kelvin, developed the absolute (Kelvin) scale from his analysis of ideal engines
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Temperatures Universe (Planck time) ~ Universe (today) ~ Average star ~ Average dust cloud ~ Planet (Mercury) ~ Planet (Neptune) ~ Planet (habitable) ~
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