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14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

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Page 1: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

14 Temperature and Heat

Lectures by James L. Pazun

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Page 2: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Goals for Chapter 14

• To study temperature and temperature scales.

• To describe thermal expansion and its applications.

• To explore and solve problems involving heat, phase changes and calorimetry.

• To study heat transfer.

• To describe solar energy and see how technology can lead to resource conservation.

Page 3: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Temperature – Figure 14.1

• Temperature is an attempt to measure the “hotness” or “coldness” on a scale you devise.

• A device to do this is called a thermometer and is usually calibrated by the melting and freezing points of a substance. This is most often water with corrections for atmospheric pressure well known.

•The thermometer is often a container filled with a substance that will expand or contract as heat flows in its surroundings.

Page 4: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Thermal equilibrium

• If two objects are placed in contact and one has more heat energy than the other, heat will always flow from hotter to colder. This will continue until both objects are at the same temperature. This condition of stability is called thermal equilibrium.

• When heat flow is considered, some materials like metals are good transmitters of heat energy. We term these materials to be thermal conductors.

• Materials like styrofoam are poor conductors of heat and will in fact, severely restrict heat flow (like the one described above). Materials that conduct of heat energy poorly are called insulators.

Page 5: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

The Zeroth Law of Thermodynamics – Figure 14.2

• Systems A, B, and C are not originally in thermal equilibrium.

• Surround A, B, and C so that they are insulated from any external influence.

•In the top figure, A and C will come to equilibrium while at the same time, B and C will also. Eventually, all three – A, B, and C will come to equilibrium. In the lower figure, only A and B will come to equilibrium.

• This is the essence of the Zeroth Law.

Page 6: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Temperature scales – Figure 14.3

• Based on the boiling and freezing points of water, two systems developed to measure temperature.

• In the United States, the Fahrenheit scale was developed with boiling at 212oF and freezing at 32oF.

• In many other countries, the Celsius (also called Centigrade) scale was developed with water freezing at 0oC and boiling at 100oC.

• Convert between them? Tf=9/5Tc+32o

• Note that the interval (degree) is smaller in the Fahrenheit scale.

Page 7: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

An absolute temperature scale – Figure 14.4

• Scientists experimenting with gases noted a linear behavior between pressure and temperature. Using various gases, the linear plots were all noted to converge at the same place (-273.15oC or 0K). → T(K) = ToC + 273.15

• Named for it’s inventor, Lord Kelvin (1827-1907), the Kelvin scale took this point to be the absolute zero of all temperatures, the point at which everything is a solid and all motion ceases.

Page 8: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Temperature conversions – Figure 14.5

• Be comfortable converting between the different temperature scales.

• Refer to Example 1 on page 445 of your text.

Page 9: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Thermal expansion – Figure 14.6

• The expansion is proportional to the original length.

• The expansion is proportional to the temperature change (for reasonable T).

Page 10: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

An interesting behavior – Figure 14.8

• Different materials expand according to their coefficients of thermal expansion.

• Refer to Table 14.1.

• Refer to Example 14.2 and Example 14.3.

Page 11: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Expansion of volume – Example 14.4

• Refers to Figure 14.9.

•Use the coefficients of thermal expansion in Table 14.2.

• The graph at right is for the expansion of water from 0-10oC.

• This is the property that allows the mercury to rise inside a thermometer.

Page 12: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Road expansion and contraction – Figure 14.10

• Refer to example 14.5 on pages 450 and 451 of your text.

Page 13: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

The mechanical equivalent of heat – Figure 14.12

• Done by James Joule in the1800’s.

• Potential energy stored in a raised mass was used to pull a cord wound on a rod mounted to a paddle in a water bath.

• The measured temperature change of the water proved the equivalence of mechanical energy and heat.

• The unit for potential energy, kinetic energy, and heat is the Joule in honor of his work.

Page 14: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Calories, calories, and joules – Figure 14.13

• The food calorie is properly noted as a kilocalorie in SI units. • A calorie is 4.184J.• So, the Big Mac you’re about to eat will cost your diet about three and a half million joules.

Page 15: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Heat capacity – Examples 14.6 and 14.7

• Substances have an ability to “hold heat” that goes to the atomic level.

• One of the best reasons to spray water on a fire is that it suffocates combustion. Another reason is that water has a huge heat capacity. Stated differently, it has immense thermal inertia. In plain terms, it’s good at cooling things off because it’s good at holding heat.

• Taking a copper frying pan off the stove with your bare hands is an awful idea because metals have almost no heat capacity. In plain terms, metals give heat away as fast as they can.

• Refer to Examples 14.6 and 14.7 on pages 453 and 454 of your text.

Page 16: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Phase changes – Figure 14.14 and the snowflake

• Which is worse to touch for a burn? 100°C water or 100°C steam? The steam, because it also contains the energy that it took to become a gas. In the case of water this is 2.3 MILLION joules per kg of water.

•The snowflake on the left needs to absorb the latent heat of fusion to become a liquid. The metal in the person’s hand to the right just did that from the person’s body temperature.

• Put ice in water. You have a refreshing drink but also solid water and liquid water in equilibrium.

Page 17: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Calorimetery – Examples 14.8 and 14.9

• Refer to the problem solving strategy 14.2 on page 458.

• Surround a system with a known amount of fluid (therefore a known heat capacity). By measuring the change in temperature you can solve for the heat evolved by the system.

Page 18: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Methods of moving heat energy – Examples 14.10-14.14

• Conduction – discussed earlier as a function of each given material. See Table 14.5 and examples 14.10-12.

• Convection – moving a heated fluid from one place to another. Our real-life examples are heated air from a furnace or heated water for a shower.

• Radiation – moving heat by electromagnetic radiation. Infrared rays from a hot burner on a stove can be felt by holding your hand over the burner. See examples 14.13-14.

Page 19: 14 Temperature and Heat Lectures by James L. Pazun Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Copyright © 2012 Pearson Education, Inc. publishing as Addison-Wesley

Solar energy and resource conservation

• This year there is a very large tax credit available for people who will install pipes over black background on the roof of their home. The initiative from the government was to provide initial momentum for the one-time cost of adding such devices to existing homes.

• The sun is ultimately the source of all energetic production on the earth but in the case of the tax credit, the plan is to harness sunlight which normally heats your roof and then escapes.

• It will be interesting to see what happens.