Paradoxical helium and sulfur hexafluoride single-breath washouts in short-term vs. sustained microgravity
Anne-Marie Lauzon 1 , G. Kim Prisk 1 , Ann R. Elliott 1 , Sylvia Verbanck 2 , Manuel Paiva 3 , and John B. West 1 1 Department of Medicine, University of California, San Diego, La Jolla, California 92093-0931; 2 Department of Pneumology Akademisch Ziekenhuis, Vrije Universiteit Brussel, 1090 Bruss...
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Veröffentlicht in: | Journal of applied physiology (1985) 1997-03, Vol.82 (3), p.859-865 |
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Zusammenfassung: | Anne-Marie
Lauzon 1 ,
G. Kim
Prisk 1 ,
Ann R.
Elliott 1 ,
Sylvia
Verbanck 2 ,
Manuel
Paiva 3 , and
John B.
West 1
1 Department of Medicine,
University of California, San Diego, La Jolla, California 92093-0931;
2 Department of Pneumology
Akademisch Ziekenhuis, Vrije Universiteit Brussel, 1090 Brussels;
and 3 Biomedical Physics
Laboratory, Université Libre de Bruxelles, 1070 Brussels, Belgium
Received 26 June 1996; accepted in final form 28 October 1996.
Lauzon, Anne-Marie, G. Kim Prisk, Ann R. Elliott, Sylvia
Verbanck, Manuel Paiva, and John B. West. Paradoxical helium and
sulfur hexafluoride single-breath washouts in short-term vs. sustained
microgravity. J. Appl. Physiol. 82(3):
859-865, 1997. During single-breath washouts in normal gravity (1 G), the phase III slope of sulfur hexafluoride
(SF 6 ) is steeper than that of
helium (He). Two mechanisms can account for this:
1 ) the higher diffusivity of He
enhances its homogeneous distribution; and
2 ) the lower diffusivity of
SF 6 results in a more peripheral
location of the diffusion front, where airway asymmetry is larger.
These mechanisms were thought to be gravity independent. However, we
showed during the Spacelab Life Sciences-2 spaceflight that in
sustained microgravity (µG) the
SF 6 -to-He slope difference is
abolished. We repeated the protocol during short periods (27 s) of µG
(parabolic flights). The subjects performed a vital-capacity
inspiration and expiration of a gas containing 5% He-1.25%
SF 6 -balance
O 2 . As in sustained µG, the
phase III slopes of He and SF 6
decreased. However, during short-term µG, the
SF 6 -to-He slope difference
increased from 0.17 ± 0.03%/l in 1 G to 0.29 ± 0.06%/l in
µG, respectively. This is contrary to sustained µG, in which the
SF 6 -to-He slope difference decreased from 0.25 ± 0.03%/l in 1 G to 0.01 ± 0.06%/l
in µG. The increase in phase III slope difference in short-term µG
was caused by a larger decrease of He phase III slope compared with that in sustained µG. This suggests that changes in peripheral gas
mixing seen in sustained µG are mainly due to alterations in the
diffusive-convective inhomogeneity of He that require >27 s of µG
to occur. Changes in pulmonary blood volume distribution or cardiogenic
mixing may explain the differences between the results found in
short-term and sustained µG.
phase III slope; inhomogeneity; convection; diffusion
0161-7567/97 $5.00
Copyright © 1997 the American Physiological Society |
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ISSN: | 8750-7587 1522-1601 |
DOI: | 10.1152/jappl.1997.82.3.859 |