PROBABILISTIC GAS AND BUBBLE DYNAMICS MODELS OF DECOMPRESSION-SICKNESS OCCURRENCE IN AIR AND NITROGEN-OXYGEN DIVING

Authors
Citation
Wa. Gerth et Rd. Vann, PROBABILISTIC GAS AND BUBBLE DYNAMICS MODELS OF DECOMPRESSION-SICKNESS OCCURRENCE IN AIR AND NITROGEN-OXYGEN DIVING, Undersea & hyperbaric medicine, 24(4), 1997, pp. 275-292
Citations number
26
ISSN journal
10662936
Volume
24
Issue
4
Year of publication
1997
Pages
275 - 292
Database
ISI
SICI code
1066-2936(1997)24:4<275:PGABDM>2.0.ZU;2-B
Abstract
Probabilistic models of the occurrence of decompression sickness (DCS) with instantaneous risk defined as the weighted sum of bubble volumes in each of three parallel-perfused gas exchange compartments were fit using likelihood maximization to the subset of the USN Primary Air an d N-2-O-2 database [n = 2,383, mean P(DCS) = 5.8%] used in development of the USN LE1 probabilistic models. Bubble dynamics with one diffusi ble gas in each compartment were modeled using the Van Liew equations with the nucleonic bubble radius, compartmental volume, compartmental bulk N-2 diffusivity, compartmental N-2 solubility, and the N-2 solubi lity in blood x compartmental blood now as adjustable parameters. Mode ls were also tested that included the effects of linear elastic resist ance to bubble growth in one, two, or all three of the modeled compart ments. Model performance about the training data and separate validati on data was compared to results obtained about the same data using the LE1 probabilistic model, which was independently implemented from pub lished descriptions. In the most successful bubble volume model, BVM(3 ), diffusion significantly slows bubble growth in one of the modeled c ompartments, whereas mechanical resistance to bubble growth substantia lly accelerates bubble resolution in all compartments. BVM(3) performe d generally on a par with LE1, despite inclusion of 12 more adjustable parameters, and tended to provide more accurate incidence-only estima tes of DCS probability than LE1, particularly for profiles in which hi gh fractional O-2 gas mixes are breathed. Values of many estimated BVM (3) parameters were outside of the physiologic range, indicating that the model emerged from optimization as a mathematical descriptor of pr ocesses beyond bubble formation and growth that also contribute to DCS outcomes. Although incomplete as a mechanistic description of DCS eti ology, BVM(3) remains applicable to a wider variety of decompressions than LE1 and affords a conceptual framework for further refinements mo tivated by mechanistic principles.