The theory of irreversible thermodynamics for reciprocating externally irre
versible cycles gives rise to an optimum efficiency at maximum power output
of eta = 1 - (T-L/T-H)(0.5) for internally reversible Carnot cycles, in co
ntrast to the upper limit for Carnot cycles of eta = 1 - (T-L/T-H) obtained
from classical thermodynamics. It is shown here in addition, for the inter
nally irreversible reciprocating Carnot cycle using linear heat transfer mo
des, that the optimum work output at maximum power (W-opt) is less than lan
d in the limit of no internal irreversibility is equal to) exactly one-half
of the work potential of the externally reversible cycle operating at maxi
mum thermal efficiency (Carnot work, W-rev) between the same temperature li
mits (i.e., W-opt less than or equal to 1/2W(rev)). To accomplish this the
analysis goes one step further than earlier works to make use of time symme
try to minimize overall cycle time and thus better optimize overall cycle p
ower. Because this novel procedure implies the concurrent use of first and
second laws of thermodynamics, it automatically ensures optimal allocation
of thermal conductances at the hot and cold ends while simultaneously achie
ving both minimization of internal entropy generation and maximization of s
pecific cycle work. Based on linear heat transfer laws, this expression for
optimum work is shown to be independent of heat conductances. (C) 2000 Els
evier Science Ltd. All rights reserved.