Journal of Applied Physiology AJP: Gastrointestinal and Liver Physiology
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J Appl Physiol 103: 737-738, 2007. First published July 19, 2007; doi:10.1152/japplphysiol.00770.2007
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INVITED EDITORIAL

Observed bubble dynamics in oxygen or heliox breathing and altitude decompression sickness

Ran Arieli

Israel Naval Medical Institute and IDF Medical Corps, Haifa, Israel

ALTITUDE decompression sickness (DCS) is a common risk in aviation and has been extensively studied over the past two decades (2, 3, 9). Attempts have been made to find a correlation between ultrasonic bubble detection and symptoms of altitude DCS (1, 8). Models extrapolating the risk of DCS from diving to altitude have not always been successful (4). Altitude DCS can occur in flying after diving, during accidental loss of cabin pressure, flying to extreme altitude, and repeated helicopter flights in intensive military operations. Denitrogenation by breathing oxygen either as a prebreathe or during decompression has been proposed as a means of reducing the risk of DCS (7, 10, 12). Exploring the effect of different treatments on the fate of altitude-induced bubbles may add to our understanding of altitude DCS and enable us to derive decompression procedures.

In a study in the Journal of Applied Physiology, Hyldegaard and Madsen (6) use their long-serving model for the observation of bubble kinetics in the tissue of the rat to explore the effect of decompression to the commonly used cabin pressure of 71 kPa. Air bubbles previously injected into adipose tissue were observed during decompression. The study supports the notion that bubbles can grow to a greater extent at low pressure and raises the question of how to reduce the risk of DCS. The authors found that compared with hypobaric air breathing, a switch to oxygen breathing had a dual effect: an initial increase in bubble volume, after which the bubble diminished and disappeared. A switch to heliox also led to bubble disappearance but prevented the large increase in volume at the outset. The time to disappearance of half of the bubbles in heliox (50:50), ~60 min from the gas switch, may be shorter (although not significantly) than it was for oxygen breathing, ~67 min. The last bubble disappeared in heliox (50:50) ~128 min after the gas switch, whereas during oxygen breathing 30% of the bubbles remained for longer than 170 min. Both of these measures point to the superiority of heliox. Thus for adipose tissue, heliox (50:50) may be preferable to oxygen, and the study therefore represents a significant contribution to the physiology of supersaturation in aviation.

It is clear that an experimental model using injected air bubbles does not represent the actual process of bubble formation during decompression. Naturally formed bubbles most probably grow from preexisting gas micronuclei. No bubbles were formed during the decompression from 101 to 71 kPa, and no DCS has been recorded in normal air transportation. Therefore, only a conservative extrapolation from the experimental model to actual flight conditions is possible. The bubbles that produce DCS are formed in both adipose and aqueous tissue. To assess the impact of altitude decompression, both adipose and aqueous tissue need to be studied.

Data from this experimental model could have a considerable impact on the use of heliox in clinical recompression therapy. It was shown in an in vitro experiment that switching the hyperbaric atmosphere from nitrogen to helium for nitrogen-saturated gelatin resulted in bubble growth (11). However, the present study (6), which agrees with previous studies from the same group, shows in contrast that the use of heliox in living tissue in an in vivo experiment causes bubble shrinkage and disappearance. This may well influence the long-standing debate regarding the use of heliox in the hyperbaric treatment of DCS.

An interesting observation is the initial bubble growth during oxygen breathing. This may have implications for aviation accidents involving the sudden loss of cabin pressure. Breathing oxygen to overcome the hypoxia will result in the growth of any decompression bubbles that have been formed and increase the risk of DCS. In such an event, it would be preferable to breathe heliox (50:50). This experimental model can be used further to explore accidental loss of cabin pressure. After decompression to extremely low pressure, both aqueous and adipose tissues would immediately be flushed with either oxygen or heliox. Immediate switching of the gas mixture is required because after half an hour at low pressure (the period of time used in the present study), most of the supersaturated dissolved gas in the aqueous tissue and half of the supersaturated gas in the adipose tissue of the rat would have been eliminated. It may well be that studies on this topic will lead to replacement of the emergency oxygen supply in aircraft by heliox. Finally, decompression models that calculate the critical gas volume for DCS risk, such as that of Flook (5), can incorporate the findings of the present and future studies to predict the risk of DCS with different gas mixtures at altitude.

This is an interesting study by Hyldegaard and Madsen (6) that prompts further investigations on aqueous tissue and with greater pressure reduction, conditions that may lead to the evolution of decompression bubbles.

FOOTNOTES


Address for reprint requests and other correspondence: R. Arieli, Israel Naval Medical Institute and IDF Medical Corps, PO Box 8040, Haifa 31080, Israel (e-mail: rarieli{at}netvision.net.il)

REFERENCES

  1. Balldin UI, Pilmanis AA, Webb JT. Pulmonary decompression sickness at altitude: early symptoms and circulating gas emboli. Aviat Space Environ Med 73: 996–999, 2002.[Medline]
  2. Balldin UI, Pilmanis AA, Webb JT. The effect of simulated weightlessness on hypobaric decompression sickness. Aviat Space Environ Med 73: 773–778, 2002.[Medline]
  3. Conkin J, Powell MR. Lower body adynamia as a factor to reduce the risk of hypobaric decompression sickness. Aviat Space Environ Med 72: 202–214, 2001.[Medline]
  4. Conkin J, Van Liew HD. Failure of the straight-line DCS boundary when extrapolated to the hypobaric realm. Aviat Space Environ Med 63: 965–970, 1992.[Medline]
  5. Flook V. The physics and physiology of decompression. Eur J Underwater Hyperbaric Med 1: 8–13, 2000.
  6. Hyldegaard O, Madsen J. Effect of hypobaric air, oxygen, heliox (50:50), or heliox (80:20) breathing on air bubbles in adipose tissue. J Appl Physiol (June 28, 2007). doi:10.1152/japplphysiol.00155.2007.
  7. Krause KM, Pilmanis AA. The effectiveness of ground level oxygen treatment for altitude decompression sickness in human research subjects. Aviat Space Environ Med 71: 115–118, 2000.[Medline]
  8. Kumar KV, Calkins DS, Waligora JM, Gilbert JH III, Powell MR. Time to detection of circulating microbubbles as a risk factor for symptoms of altitude decompression sickness. Aviat Space Environ Med 63: 961–964, 1992.[Medline]
  9. Pilmanis AA, Webb JT, Kannan N, Balldin U. The effect of repeated altitude exposures on the incidence of decompression sickness. Aviat Space Environ Med 73: 525–531, 2002.[Medline]
  10. Rice GM, Vacchiano CA, Moore JL Jr, Anderson DW. Incidence of decompression sickness in hypoxia training with and without 30-min O2 prebreathe. Aviat Space Environ Med 74: 56–61, 2003.[Medline]
  11. Strauss RH, Kunkle TD. Isobaric bubble growth: a consequence of altering atmospheric gas. Science 186: 443–444, 1974.[Abstract/Free Full Text]
  12. Webb JT, Pilmanis AA, Kannan N, Olson RM. The effect of staged decompression while breathing 100% oxygen on altitude decompression sickness. Aviat Space Environ Med 71: 692–698, 2000.[Medline]




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