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Figure 20.1  Joule’s experiment for determining the mechanical equivalent of heat. The falling blocks rotate the paddles, causing the temperature of the.

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Presentation on theme: "Figure 20.1  Joule’s experiment for determining the mechanical equivalent of heat. The falling blocks rotate the paddles, causing the temperature of the."— Presentation transcript:

1 Figure 20.1  Joule’s experiment for determining the mechanical equivalent of heat. The falling blocks rotate the paddles, causing the temperature of the water to increase. Fig. 20.1, p.607

2 Table 20.1, p.608

3 Table 20.2, p.612

4 Figure 20. 2 A plot of temperature versus energy added when 1
Figure 20.2  A plot of temperature versus energy added when 1.00 g of ice initially at –30.0°C is converted to steam at 120.0°C. Fig. 20.2, p.612

5 Figure 20.3  Work is done on a gas contained in a cylinder at a pressure P as the piston is pushed downward so that the gas is compressed. Fig. 20.3, p.615

6 Active Figure 20.4  A gas is compressed quasi-statically (slowly) from state i to state f. The work done on the gas equals the negative of the area under the PV curve. At the Active Figures link at you can compress the piston in Figure 20.3 and see the result on the PV diagram of this figure. Fig. 20.4, p.616

7 Active Figure 20.5  The work done on a gas as it is taken from an initial state to a final state depends on the path between these states. At the Active Figures link at you can choose one of the three paths and see the movement of the piston in Figure 20.3 and of a point on the PV diagram of this figure. Fig. 20.5, p.617

8 Active Figure 20.5  The work done on a gas as it is taken from an initial state to a final state depends on the path between these states. At the Active Figures link at you can choose one of the three paths and see the movement of the piston in Figure 20.3 and of a point on the PV diagram of this figure. Fig. 20.5a, p.617

9 Active Figure 20.5  The work done on a gas as it is taken from an initial state to a final state depends on the path between these states. At the Active Figures link at you can choose one of the three paths and see the movement of the piston in Figure 20.3 and of a point on the PV diagram of this figure. Fig. 20.5b, p.617

10 Active Figure 20.5  The work done on a gas as it is taken from an initial state to a final state depends on the path between these states. At the Active Figures link at you can choose one of the three paths and see the movement of the piston in Figure 20.3 and of a point on the PV diagram of this figure. Fig. 20.5c, p.617

11 Figure 20.6  (a) A gas at temperature Ti expands slowly while absorbing energy from a reservoir in order to maintain a constant temperature. (b) A gas expands rapidly into an evacuated region after a membrane is broken. Fig. 20.6, p.617

12 Figure 20.6  (a) A gas at temperature Ti expands slowly while absorbing energy from a reservoir in order to maintain a constant temperature. Fig. 20.6a, p.617

13 Figure 20.6  (b) A gas expands rapidly into an evacuated region after a membrane is broken.
Fig. 20.6b, p.617

14 Active Figure 20.7  The first law of thermodynamics equates the change in internal energy Eint in a system to the net energy transfer to the system by heat Q and work W. In the situation shown here, the internal energy of the gas increases. At the Active Figures link at you can choose one of the four processes for the gas discussed in this section and see the movement of the piston and of a point on a PV diagram. Fig. 20.7, p.619

15 Figure 20.8  The PV diagram for an isothermal expansion of an ideal gas from an initial state to a final state. The curve is a hyperbola. Fig. 20.8, p.621

16 Figure 20.9  Identify the nature of paths A, B, C, and D.
Fig. 20.9, p.621

17 UN-20. 01 A pan of boiling water sits on a stove burner
UN A pan of boiling water sits on a stove burner. Energy enters the water through the bottom of the pan by thermal conduction. (Charles D. Winters) Fig. 20.UN, p.623

18 Figure 20.10  Energy transfer through a conducting slab with a cross-sectional area A and a thickness ∆x. The opposite faces are at different temperatures Tc and Th. Fig , p.623

19 Table 20.3, p.624

20 Figure 20.11  Conduction of energy through a uniform, insulated rod of length L. The opposite ends are in thermal contact with energy reservoirs at different temperatures. Fig , p.624

21 Figure Energy transfer by conduction through two slabs in thermal contact with each other. At steady state, the rate of energy transfer through slab 1 equals the rate of energy transfer through slab 2. Fig , p.625

22 Figure 20.13  In which case is the rate of energy transfer larger?
Fig , p.626

23 Table 20.4, p.627

24 Figure 20.14  An exterior house wall containing (a) an air space and (b) insulation.
Fig , p.627

25 Figure 20.15  Convection currents are set up in a room heated by a radiator.
Fig , p.628

26 Figure 20.16  A cross-sectional view of a Dewar flask, which is used to store hot or cold substances.
Fig , p.629

27 Alternating patterns on a snow-covered roof.
Fig. Q20.14, p.631

28 Fig. P20.23, p.634

29 Fig. P20.24, p.634

30 Fig. P20.30, p.634

31 Fig. P20.32, p.634

32 Fig. P20.33, p.635

33 Fig. P20.38, p.635

34 Fig. P20.40, p.635

35 Fig. P20.43, p.635

36 Fig. P20.63, p.637

37 Fig. P20.65, p.637

38 Fig. P20.67, p.638

39 Fig. P20.69, p.638

40 Fig. P20.70, p.638

41 Fig. QQA20.3, p.639


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