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Botkin Environmental Science Earth as Living Planet 8th txtbk

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290 CHAPTER 14 Energy: Some B<strong>as</strong>ics<br />

and other energy forms, including electricity to charge the<br />

battery and play the radio.<br />

Why can’t we collect the w<strong>as</strong>ted heat and use it to run<br />

the engine? Again, <strong>as</strong> the second law of thermodynamics<br />

tells us, once energy is degraded to low-quality heat, it can<br />

never regain its original availability or energy grade. When<br />

we refer to low-grade heat energy, we mean that relatively<br />

little of it is available to do useful work. High-grade energy,<br />

such <strong>as</strong> that of g<strong>as</strong>oline, coal, or natural g<strong>as</strong>, h<strong>as</strong> high<br />

potential to do useful work. The biosphere continuously<br />

receives high-grade energy from the sun and radiates lowgrade<br />

heat to the depths of space. 3, 4<br />

1 Energy is all potential.<br />

2 Energy is all kinetic.<br />

3 Energy is potential and kinetic.<br />

1 1<br />

3 2 3<br />

FIGURE 14.3 Diagram of a tire swing, illustrating the relation<br />

between potential and kinetic energy.<br />

heat energy thus generated back into potential energy. Energy<br />

is conserved in the tire swing. When the tire swing<br />

finally stops, all the initial gravitational potential energy h<strong>as</strong><br />

been transformed by way of friction to heat energy. If the<br />

same amount of energy, in the form of heat, were returned<br />

to the tire swing, would you expect the swing to start again?<br />

The answer is no! What, then, is used up? It is not energy<br />

because energy is always conserved. What is used up is the<br />

energy quality—the availability of the energy to perform<br />

work. The higher the quality of the energy, the more e<strong>as</strong>ily<br />

it can be converted to work; the lower the energy quality,<br />

the more difficult to convert it to work.<br />

This example illustrates another fundamental<br />

property of energy: Energy always tends to go from<br />

a more usable (higher-quality) form to a less usable<br />

(lower-quality) form. This is the second law of<br />

thermodynamics, and it means that when you use<br />

energy, you lower its quality.<br />

Let’s return to the example of the stalled car, which<br />

you have now pushed to the side of the road. Having<br />

pushed the car a little way uphill, you have incre<strong>as</strong>ed its<br />

potential energy. You can convert this to kinetic energy<br />

by letting it roll back downhill. You engage the gears to<br />

restart the car. As the car idles, the potential chemical energy<br />

(from the g<strong>as</strong>oline) is converted to w<strong>as</strong>te heat energy<br />

14.3 Energy Efficiency<br />

Two fundamental types of energy efficiencies are derived<br />

from the first and second laws of thermodynamics: first-law<br />

efficiency and second-law efficiency. First-law efficiency<br />

deals with the amount of energy without any consideration<br />

of the quality or availability of the energy. It is calculated<br />

<strong>as</strong> the ratio of the actual amount of energy delivered where<br />

it is needed to the amount of energy supplied to meet that<br />

need. Expressions for efficiencies are given <strong>as</strong> fractions;<br />

multiplying the fraction by 100 converts it to a percentage.<br />

As an example, consider a furnace system that keeps a home<br />

at a desired temperature of 18°C (65°F) when the outside<br />

temperature is 0°C (32°F). The furnace, which burns natural<br />

g<strong>as</strong>, delivers 1 unit of heat energy to the house for every<br />

1.5 units of energy extracted from burning the fuel. That<br />

means it h<strong>as</strong> a first-law efficiency of 1 divided by 1.5, or<br />

67% (see Table 14.1 for other examples). 4 The “unit” of<br />

energy for our furnace is arbitrary for the purpose of discussion;<br />

we also could use the British thermal unit (Btu) or<br />

some other units (see A Closer Look 14.1).<br />

First-law efficiencies are misleading because a high value<br />

suggests (often incorrectly) that little can be done to save energy<br />

through additional improvements in efficiency. This problem<br />

is addressed by the use of second-law efficiency. Secondlaw<br />

efficiency refers to how well matched the energy end use<br />

is with the quality of the energy source. For our home-heating<br />

example, the second-law efficiency would compare the minimum<br />

energy necessary to heat the home to the energy actually<br />

used by the g<strong>as</strong> furnace. If we calculated the second-law<br />

efficiency (which is beyond the scope of this discussion), the<br />

result might be 5%—much lower than the first-law efficiency<br />

of 67%. 4 (We will see why later.) Table 14.1 also lists some<br />

second-law efficiencies for common uses of energy.<br />

Values of second-law efficiency are important because<br />

low values indicate where improvements in energy technology<br />

and planning may save significant amounts of highquality<br />

energy. Second-law efficiency tells us whether the<br />

energy quality is appropriate to the t<strong>as</strong>k. For example, you<br />

could use a welder’s acetylene blowtorch to light a candle,<br />

but a match is much more efficient (and safer <strong>as</strong> well).

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