It is acknowledged that the Curzon-Ahlborn efficiency eta(CA) determines th
e efficiency at maximum power production of heat engines only affected by t
he irreversibility of finite rate heat transfer (endoreversible engines), b
ur PICA is not the upper bound of the efficiencies of heat engines. This is
conceptually different from the role of the Carnot efficiency eta(C) which
is indeed the upper bound of the efficiencies of all heat engines. Some au
thors have erroneously criticized eta(CA) as if it were the upper bound of
the efficiencies of endoreversible heat engines. Although the efficiencies
of real heat engines cannot attain the Carnot efficiency, it is possible, a
nd often desirable, for their efficiencies to be larger than their respecti
ve maximum power efficiencies, In fact, the maximum power efficiency is the
allowable lower bound of the efficiency for a given class of heat engines.
These important conclusions may be expounded clearly by the theory of fini
te time thermodynamics. (C) 2000 Published by Elsevier Science Ltd.