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Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley PowerPoint ® Lectures for University Physics, Twelfth Edition Hugh D. Young and Roger A. Freedman Lectures by James Pazun Chapter 17 Temperature and Heat

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Page 1: Temperature and Heat - University of California, Santa … © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley PowerPoint ®Lectures ... Copyright © 2008 Pearson

Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley

PowerPoint® Lectures for

University Physics, Twelfth Edition

– Hugh D. Young and Roger A. Freedman

Lectures by James Pazun

Chapter 17

Temperature and Heat

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Goals for Chapter 17

• To delineate the three different temperature scales

• To describe thermal expansion and thermal stress

• To consider heat, phase changes, and calorimetry

• To study how heat flows with convection,

conduction, and radiation

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Introduction

• Growing up in Pittsburgh, molten steel was a common sight. Still it is imposing at 1500oC.

• The worst common burns you can imagine are steam burns. You have not only water heated to its boiling point but gaseous steam carrying the heat of vaporization. It’s a great deal of energy in a small space.

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Measuring temperature

• There are many ways to measure

temperature, but the two devices

mentioned below take advantage of

a gas or liquid sample which

expands if heat is added and

contracts if heat is removed.

• A cylinder of gas will show pressure

rise if volume is kept constant.

• A small container of liquid will see

the liquid increase in volume as

temperatures rise. Mercury was

chosen “early on” because it’s so

dense, a small volume can record

large temperature ranges.

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The zeroth law of thermodynamics

• Simply stated? “Heat will always travel from a hot reservoir to a cold one without outside energy forcing an unnatural transfer.”

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Thermometers? Just our way of trying to see where the heat is

• The measure of temperature is a way of expressing how much heat one object is holding relative to another.

• There are several examples shown at right. You can base a thermometer on thermal expansion of a gas, differential expansion of bimetal strips, even on something as wild as laser-doppler shift.

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The coldest we can ever get?

• Early experiments observed changes in pressure or volume as

temperature changed.

• It was noticed that the linear trends lead to a consistent lowest

temperature that we call “absolute zero”—labeled 0K after Lord Kelvin.

• Refer to Example 17.1.

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Conversions are expected

• Values on the temperatures scales (Fahrenheit, Centigrade/Celsius,

and Kelvin) may be readily interconverted. Physics professors will

want values to eventually be in Kelvins because that’s the form in

SI units.

• See Figure 17.7 below.

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Thermal expansion—linear

• A change in

length will

accompany a

change in

temperature.

The size of the

change will

depend on the

material.

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Changing temperature changes atomic spacing

• Molecules can be visualized as bedsprings and spheres. More

heat (higher temperatures) is reflected by the motion of the

atoms relative to each other.

• See Figure 17.9 below.

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Coefficients of expansion

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Thermal changes in material length and volume

• Refer to Problem-Solving Strategy 17.1.

• Consult Example 17.2 (change in length).

• Consult Example 17.3 (change in length II).

• Consult Example 17.4 (change in volume).

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Thermal expansion we see constantly

• Water is interesting. There are no

other liquids that expand to become

less dense as a solid than they are

as a liquid. This is fortunate, if

lakes were to freeze and dense ice

sink to the bottom, everything in

the water would die as the liquid

became solid from the bottom up.

• Thermal expansion joints allow

roads to expand and contract

without any stress to the material

used to build.

• Refer to Example 17.5.

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James Joule and the mechanical equivalent of heat

• Joule knew a mass

above the ground had

potential energy. He

dropped an object on a

cord, turning a paddle

in water monitored by

a very accurate

thermometer.

• His conclusion was to

connect energy

conservation (potential

and kinetic) to heat as

a third form observed.

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Specific heat

• A specific heat value reveals

how much temperature will

change when a given amount of

a substance absorbs a given

amount of heat.

• Water is a “benchmark” as one

ml of water will absorb 1 cal of

heat to raise its temperature by

1oC.

• Refer to Example 17.6 and

Example 17.7.

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Specific heat values

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Phase changes and temperature behavior

• A solid will absorb heat according to its heat

capacity, becoming a hotter solid.

• At the melting point, a solid will absorb its

heat of fusion and become a liquid. An

equilibrium mixture of a substance in both its

liquid and solid phases will have a constant

temperature.

• A cold liquid will absorb heat according to its

heat capacity to become a hotter liquid.

• At the boiling point, a liquid will absorb its

heat of vaporization and become a gas. An

equilibrium mixture of liquid and gas will have

a constant temperature.

• A cold gas can absorb heat according to its heat

capacity and become a hotter gas.

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Heats of Fusion and Heats of Vaporization

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Using well-behaved water to measure other systems

• Because water is a good thermal sink, is readily available, and reproducibly absorbs 4.184 J for every gram to rise in temperature by 1oC, it is often used to measure another object’s change in heat energy by comparison.

• For example, an unknown metal might be massed, raised to a known temperature (say to 100oC in a boiling water bath), then added to a known amount of cold water. The resulting change in the temperature of the water will allow heat absorbed to be calculated and then the heat capacity of the unknown metal.

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Heat calculations

• Follow Problem-Solving Strategy 17.2.

• Refer to Example 17.8 (no phase change).

• Refer to Example 17.9 (changes in both temperature and

phase).

• Refer to Example 17.10 (an example that could be done in a

kitchen).

• Refer to Example 17.11 (combustion, temperature change,

and phase change).

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Why, and how well, do materials transfer heat?

• Figure 17.23 illustrates

the model.

• Table 17.5 lists thermal

conductivities. They are

dramatically different,

from very large values

for conductors like

metals to very small

values for insulators

like styrofoam or wood.

• Consider Problem-

Solving Strategy 17.3.

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Thermal conductivity

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Thermal Conductivity – Lattice Waves – Longitudinal and Transverse

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Thermal Conductivity – k (watts/m-Kelvin)

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Conduction of heat I

• Consider Example 17.12.

• What makes a picnic

cooler effective?

• Figure 17.25 at right

illustrates the problem.

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Conduction of heat II

• Consider Example 17.13.

• This is a good reason not to pick up a metal frying pan by

its bare handle.

• Figure 17.26 below illustrates the problem.

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Conduction of heat III

• Consider Example 17.14.

• There are variations of the metal bar problem.

• Figure 17.27 below illustrates the problem.

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Convection of heat

• Heating by moving large

amounts of hot fluid,

usually water or air.

• Figure 17.28 at right

illustrates heat moving by

convection.

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Radiation of heat

• Infrared lights, hot metal

objects, a fireplace,

standing near a running

furnace … these are all

objects heating others by

broadcast of EM radiation

just lower in energy than

visible red.

• Consider Example 17.15.

• Consider Example 17.16.