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Temperature Physics 313 Professor Lee Carkner Lecture 2

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Temperature. Physics 313 Professor Lee Carkner Lecture 2. 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 - PowerPoint PPT Presentation

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Page 1: Temperature

Temperature

Physics 313Professor Lee

CarknerLecture 2

Page 2: Temperature

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

Page 3: Temperature

Macroscopic Microscopic

Specify a few basic bulk properties

Classical Thermodynamics

Specify states of individual units

Statistical mechanics

Page 4: Temperature

Systems Material separated from its

surroundings by a boundary

Closed

e.g. gas in a piston Open

e.g. an automobile radiator

Page 5: Temperature

Processes State

Process

Quasi - Static (Quasi-Equilibrium) Process

slow changes Non-quasi static processes are discontinuous

Page 6: Temperature

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

Page 7: Temperature

System Boundaries Adiabatic Wall

thermal insulator Dithermal wall

thermal conductor

Page 8: Temperature
Page 9: Temperature

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)

Page 10: Temperature

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

Page 11: Temperature

Typical “toothed” bridge expansion joint

Page 12: Temperature

“Rocker” support that allows deck expansion

Page 13: Temperature

“Sleeved” railing expansion section

Page 14: Temperature

The Brooklyn Bridge

Page 15: Temperature

The Brooklyn Bridge 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

Page 16: Temperature

Brooklyn Bridge cables

Page 17: Temperature

Stringing the Cables

Page 19: Temperature

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

Page 20: Temperature

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

Page 21: Temperature
Page 22: Temperature

Isotherms Plot pressure and volume

Curve is called an isotherm

Temperature determines thermal equilibrium

Page 23: Temperature
Page 24: Temperature

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

Page 25: Temperature

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

Page 26: Temperature

Temperatures Universe (Planck time) ~ Universe (today) ~ Average star ~ Average dust cloud ~ Planet (Mercury) ~ Planet (Neptune) ~ Planet (habitable) ~