Ya, and as we all *cough* know it is melting the polar ice caps and causing the sea to swallow up coastal states. Which means all scuba divers should start paying a tax for every breath they exhale.
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And your point is?
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Ya, and as we all *cough* know it is melting the polar ice caps and causing the sea to swallow up coastal states. Which means all scuba divers should start paying a tax for every breath they exhale.
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@Mr Carcharodon: I think you misunderstood my last post. I bold-faced the text that I had issues with. I would be satisfied if you could tell me what tissue in the human body correlates with the "slow" compartment and how perfusion rate can be accurately measured through that specific compartment. You made the following statement:So if you have an unsaturated tissue and pump more nitrogen into it by increasing the perfusion of that tissue what do you suppose that does to the time constant of that tissue? The idea that tissue time constants are dependent on perfusion goes back to Haldane’s paper in 1908. If you want a more quantitative approach I would suggest Hennessy’s paper (Bulletin of Mathematical Biology 36, 5, October 1974). Or there is an overview of the effects of blood flow on gas loading in chapter XIII of Mike Powell's Decompression Physiology syllabus.
Also take a look at Gene's post #14 above.
I maintain that there is no way that you can know that. You are applying a quantifiable biophysical property (blood perfusion rate) to a component of a mathematical model....the slowest tissues do not vary much in perfusion rates with activity...
I would be satisfied if you could tell me what tissue in the human body correlates with the "slow" compartment and how perfusion rate can be accurately measured through that specific compartment.
The body consists of various types of tissue. The rate at which an inert gas is absorbed (loaded) by each tissue during hyperbaric exposure, and subsequently released (off-loaded or off-gassed) during decompression, depends on several factors. These include the blood perfusion in the tissue and the solubility of the gas in each particular tissue type. A simplified description of tissues is that they can be fast or slow at absorbing and releasing inert gas. The following examples of the 'speed' at which this process can occur for several tissue types exposed to both nitrogen and helium - the two most commonly used inert gasses in diving.
Tissue Half-time, Nitrogen (mins) Half-time, Helium (mins)
Spinal Cord 12.5 12.5
Skin, Muscle 37 - 79 14 - 30
Inner Ear 146 - 238 55 - 90
Joints, Bones 304 - 635 115 - 240
Edmonds, Lowry and Pennefather (1991)
@Puffer Fish: I don't understand how the equivalent N and He half-time numbers for spinal cord represent a "major violation of several gas permeability laws." Spinal cord tissue is comprised of a highly heterogeneous mix of neurons and various glial cells.In particular the spinal cord.. where it shows equal numbers. That would be one major violation of several gas permeablity laws...wonder if that was a measure of the fluid in the spnal cord... which would be possible. In that case, one would be measuring the huge space, in cellular terms between two gradients, with slow migration in on one side and fast movement on the other, leaving the middle fairly low, as long as one is not near saturation....
Do you know how Edmonds et al. arrived at these data? Was it done in the human system?
And due to the higher rate of breathing, the air will spend less time in the lungs and less time in contact with the tissues that transfer the nitrogen into the blood stream.
It must be right that if you put a larger amount of gas through the alveolar tissues during a dive (ie. through breathing harder due to exertion), greater exposure would equal greater absorbtion.
After all, we know that divers can do a five minute dive which descends to 800 feet and ascend directly to the surface (at considerably faster than 60 feet a minute) with no decompression stops and not suffer DCS, provided that they only utilise one lungful of air.