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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 water to increase. Fig. 20.1, p.607
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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 water to increase. Fig. 20.1, p.607
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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
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Table 20.1, p.608
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Table 20.2, p.612
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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
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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
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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
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Active Figure 22. 11 PV diagram for the Carnot cycle
Active Figure 22.11 PV diagram for the Carnot cycle. The net work done Weng equals the net energy transferred into the Carnot engine in one cycle, |Qh| – |Qc|. Note that ∆Eint = 0 for the cycle. At the Active Figures link at you can observe the Carnot cycle on the PV diagram while you also observe the motion of the piston in Figure Fig , p.676
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Active Figure 22. 11 PV diagram for the Carnot cycle
Active Figure 22.11 PV diagram for the Carnot cycle. The net work done Weng equals the net energy transferred into the Carnot engine in one cycle, |Qh| – |Qc|. Note that ∆Eint = 0 for the cycle. At the Active Figures link at you can observe the Carnot cycle on the PV diagram while you also observe the motion of the piston in Figure
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Figure 20.14 An exterior house wall containing (a) an air space and (b) insulation.
Fig , p.627
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Figure 20.15 Convection currents are set up in a room heated by a radiator.
Fig , p.628
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Figure 20.16 A cross-sectional view of a Dewar flask, which is used to store hot or cold substances.
Fig , p.629
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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
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Table 20.3, p.624
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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
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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
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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
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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
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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
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Figure 20.6 (b) A gas expands rapidly into an evacuated region after a membrane is broken.
Fig. 20.6b, p.617
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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
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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
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Figure 20.9 Identify the nature of paths A, B, C, and D.
Fig. 20.9, p.621
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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
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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
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Table 20.3, p.624
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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
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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
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Figure 20.13 In which case is the rate of energy transfer larger?
Fig , p.626
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Table 20.4, p.627
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Alternating patterns on a snow-covered roof.
Fig. Q20.14, p.631
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Fig. P20.23, p.634
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Fig. P20.24, p.634
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Fig. P20.30, p.634
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Fig. P20.32, p.634
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Fig. P20.33, p.635
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Fig. P20.38, p.635
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Fig. P20.40, p.635
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Fig. P20.65, p.637
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Fig. P20.67, p.638
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Fig. P20.69, p.638
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Fig. P20.70, p.638
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Fig. QQA20.3, p.639
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