Well, took a couple of hours to pull these together but I think it will help a few of you on your quest...
The first use of the term 'oxygen window' is by Albert Behnke [1]. Behnke also refers to early work by Momsen on 'partial pressure vacancy' (PPV) [2] where he used partial pressures of O2 and He as high as 2-3 ATA to create a maximal PPV [3]. Behnke then goes on to describe 'Isobaric inert gas transport' or 'inherent unsaturation' as termed by LeMessurier and Hills [4] and Hills [5, 6] who made independent observations at the same time. Van Liew et. al. also made a similar observation that they did not name at the time [7]. The clinical significance of their work was later shown by Sass [8]
The 'oxygen window' effect in decompression has been described by many authors and the limits reviewed by Van Liew et. al. in 1993 [9]. The following passage is quoted from their Technical Note [9]:
Van Liew et. al.:
When living animals are in steady state, the sum of the partial pressures of dissolved gases in the tissues is usually less than atmospheric pressure, a phenomenon known as the "oxygen window", "partial pressure vacancy" or "inherent unsaturation" [1, 7, 10, 11]. This is because metabolism lowers partial pressure of O2 in tissue below the value in arterial blood and the binding of O2 by hemoglobin causes a relatively large PO2 difference between tissues and arterial blood. Production of CO2 is usually about the same as consumption of O2 on a mole-for-mole basis, but there is little rise of PCO2 because of its high effective solubility. Levels of O2 and CO2 in tissue can influence blood flow and thereby influence washout of dissolved inert gas, but the magnitude of the oxygen window has no direct effect on inert-gas washout. The oxygen window provides a tendency for absorption of the gas quantities in the body such as pneumothoraces or decompression sickness (DCS) bubbles [7]. With DCS bubbles, the window is a major factor in the rate of bubble shrinkage when the subject is in a steady state, modifies bubble dynamics when inert gas is being taken up or given off by the tissues, and may sometimes prevent the transformation of bubble nuclei into stable bubbles [12].
This paper then goes on to describe the measurements important to evaluating the oxygen window as well as simplify the "assumptions available for the existing complex anatomical and physiological situation to provide calculations, over a wide range of exposures, of the oxygen window" [9]. (abstract summarizes the results)
1. Behnke. (1967) The isobaric (oxygen window) principle of decompression. In: The New Thrust Seaward. Trans. Third Marine Tech. Soc. Conf. 5-7 June, San Diego. Washington, DC: Marine Tech. Soc. RRR ID:
4029
2. Momsen. (1942) Report on Use of Helium Oxygen Mixtures for Diving. US Naval Experimental Diving Unit Washington, DC Technical Report 42-02. RRR ID:
3312
3. Behnke. (1969) Early Decompression Studies. In: The Physiology and Medicine of Diving and Compressed Air Work, Bennett and Elliott. First Edition. p234
4. Hills. (1965) Decompression Sickness. A thermodynamic approach arising from a study on Torres Strait diving techniques. Hvalradets Skrifter, Nr. 48, 54-84.
5. Hills. (1966) A thermodynamic and kinetic approach to decompression sickness. Thesis
6. Hills. (1978) A fundamental approach to the prevention of decompression sickness. South Pacific Underwater Medicine Society Volume 8 Number 2. RRR ID:
6176
7. Van Liew HD, Bishop B, Walder P, Rahn H. (1965) Effects of compression on composition and absorption of tissue gas pockets. J Appl Physiol. 1965 Sep;20(5):927-33. PMID:
5837620
8. Sass (1976) Minimum <delta>P for bubble formation in pulmonary vasculature. Abstract of the Undersea and Hyperbaric Medical Society, Inc. Annual Scientific Meeting held May 12-13, 1976. Carillon Hotel, Miami Beach, FL. RRR ID:
5257
9. Van Liew HD, Conkin J, Burkard ME. (1993) The oxygen window and decompression bubbles: estimates and significance. Aviat Space Environ Med. 1993 Sep;64(9 Pt 1):859-65. PMID:
8216150
10. Hills. (1977) Decompression Sickness. The biophysical basis of prevention and treatment. New York: John Wiley, 1977:239-43.
11. Vann. (1982) Decompression theory and applications. In: Bennett PB, Elliott DH eds. The physiology and medicine of diving. 3rd ed. London: Bailliere Tindall, 1982; 352-82.
12. Van Liew. (1991) Simulation of the dynamics of decompression sickness bubbles and the generation of new bubbles. Undersea Biomed Res. 1991 Jul;18(4):333-45. RRR ID:
2592
Other articles of interest:
-- Hills and LeMessurier. Unsaturation in living tissue relative to the pressure and composition of inhaled gas and its significance in decompression theory. Clin Sci. 1969 Apr;36(2):185-95.
-- Yount and Lally. On the use of oxygen to facilitate decompression. Aviat Space Environ Med. 1980; 51:544-50.
-- Reinertsen, R. E., V. Flook, S. Koteng, and A. O. Brubakk. Effect of oxygen tension and rate of pressure reduction during decompression on central gas bubbles. J. Appl. Physiol. 84(1): 351-356, 1998.
*and third Conkin ref in 24 hours so I am done for a while... :14: