The lung transports oxygen (O2) from outside to the
alveolar space
and carbon dioxide (CO2) the other way around. This is by a
convective process
since it implies actual gas flow. That is not possible
between lung air and blood; here, it is by diffusion. Diffusion is very
effective on short distances but completely inadequate over longer ones;
as explained in this page. So, between lung
and the various tissues, blood has to flow carrying O2 and CO2
to and from – convection. No flow within tissues, so diffusive transport
there.
The figure is extremely simplified but is for an overall idea and as a basis for modelling. Most important: it takes some time between lung and tissues. A blood flow of 5 L/min and a blood volume of 5 L implies a 1 minute cycle time, so, on average half a minute delay. This makes coupling between metabolism and ventilation slow, and has consequences for the regulations: these would become unstable if too fast.
It complicates modelling of lung gas values for changing metabolism, e.g., when someone starts heavy work. Note, that this half minute is an average – for tissue distant from the lung, as leg muscle, it will even be more. So, the delay even is heterogeneous too: some CO2 arrives after a couple of seconds, some after a minute.
Again, modelling is through the gas law. In both the blood-lung and the blood-tissue transfer, all CO2 produced in the tissue has to be exchanged leading to:
PTot˙VCO2 = ˙nCO2RT = Q (cv,CO2 − ca,CO2)RT |
The main concern of ventilation regulation is on CO2; O2 mostly is no problem. Transfer modelling is the same as for CO2:
PTot˙VO2 = ˙nO2RT = Q cHb(Sa,CO2 − Sv,CO2)RT |