To examine the effect of quantum degeneracy on the cycle efficiency, Stirli
ng power cycles working with ideal Bose and Fermi gases are thermodynamical
ly analysed. These cycles are called Bose and Fermi cycles. Efficiency expr
essions of Bose and Fermi cycles are derived (eta (B) and eta (F) respectiv
ely). Variations of them with the temperature ratio (tau = T-L/T-H) and spe
cific volume ratio (r(v) = v(H)/v(L)) are examined. Efficiencies are compar
ed with each other and that of the classical Stirling cycle (eta (C)) It is
shown that eta (F) and eta (B) depend on both temperatures and specific vo
lumes of the cycle although eta (C) depends on only the temperatures of the
cycle. It is also seen that eta (F) < eta (B) < eta (C). The quantities De
lta eta (F) = eta (C) - eta (F) and Delta eta (B) = eta (C) - eta (B) go to
zero at the classical gas conditions. Under degeneracy gas conditions, how
ever, Delta eta (B) is greater than zero and it has one maximum and one min
imum value while TL decreases. On the other hand, Delta eta (F) has no extr
emum point and increases continuously with decreasing T-L. eta (F) and eta
(B) decrease with increasing r(v) when v(H) is constant although they incre
ase when v(L) is constant. Under the conditions that the working gas remain
s a completely degenerate Bose gas throughout the cycle, it is seen that et
a (B) goes to 0.4 instead of unity when tau goes to zero.