About \(86 \%\) of the world's electrical energy is produced by using steam
turbines, a form of heat engine. In his analysis of an ideal heat engine, Sadi
Carnot concluded that the maximum possible efficiency is defined by the total
work that could be done by the engine, divided by the quantity of heat
available to do the work (for example, from hot steam produced by combustion
of a fuel such as coal or methane). This efficiency is given by the ratio
\(\left(T_{\text {hyda }}-T_{\text {low }}\right) / T_{\text {high }}\). where
\(T_{\text {bigh }}\) is the temperature of the heat going into the engine and
\(T_{\text {low }}\) is that of the heat leaving the engine, (a) What is the
maximum possible efficiency of a heat engine operating between an input
temperature of \(700 \mathrm{~K}\) and an exit temperature of \(288 \mathrm{~K}\)
? (b) Why is it important that electrical power plants be located near bodies
of relatively cool water? (c) Under what conditions could a heat engine
operate at or near \(100 \%\) efflciency? (d) It is often said that if the
energy of combustion of a fuel such as methane were captured in an electrical
fuel cell instead of by burning the fuel in a heat engine, a greater fraction
of the energy could be put to useful work. Make a qualitative drawing like
that in Figure \(5.10\) (p. 175) that illustrates the fact that in principle the
fuel cell route will produce more useful work than the heat engine route from
combustion of methane.