Alveolar gas transfer over a given breath (i) was determined in ten subject
s at rest and during steady-state cycling at 60, 90 or 120 W as the sum of
volume of gas transferred at the mouth plus the changes of the alveolar gas
stores. This is given by the gas fraction (F-A) change at constant volume
plus the volume change (DeltaV(Ai)) at constant fraction i.e. VAl-1(F-Ai-FA
i-1)+F-Ai.(Delta VAi), where VAi-1 is the end-expiratory volume at the begi
nning of the breath. These quantities, except for VAi-1 can be measured on
a single-breath (breath-by-breath) basis and VAi-1 equal to the subject's f
unctional residual capacity (FRC, Auchincloss model). Alternatively, the re
spiratory cycle can be defined as the interval elapsing between two equal e
xpiratory gas fractions in two successive breaths (Gronlund model G). In th
is case, F-t1=F-t2 and thus the term VAi-1 (F-Ai-FAi-1) vanishes. In the pr
esent study, average alveolar O-2 uptake ((V) over dot O-2,O-A) and CO2 out
put ((V) over dot CO2,A) were equal in both approaches whereby the mean sig
nal-to-noise ratio (S/N) was 40% larger in G. Other approaches yield steady
state S/N values equal to that obtained in G, although they are based on t
he questionable assumption that the inter-breath variability of alveolar ga
s transfer is minimal. It is concluded that the only promising approach for
assessing "true" single breath alveolar gas transfer is that originally pr
oposed by Gronlund.