Oxygen transport between the lungs and the body depends on numerous complex factors. Ventilation and the alveolar-capillary surface area are of course important but a critical component is hemoglobin. Oxygen is poorly soluble in water (which is what blood is mostly made of) and the transportation of oxygen throughout the body would not happen without hemoglobin’s ability to absorb and release oxygen on demand. Although it is possible to measure the diffusing capacity of oxygen (DLO2) the process is technically difficult and not at all suited to routine clinical testing.
There are a number of gases that are able to diffuse across the alveolar-capillary membrane and can be used in a variety of physiological measurements but in order for a particular gas to act as a substitute for oxygen it must be able to interact with hemoglobin. Carbon monoxide (CO) has an affinity for hemoglobin approximately 220 times greater than oxygen and was the first gas used to measure diffusing capacity (DLCO). DLCO has been a routine test for well over 50 years and has been measured by single-breath, steady-state and rebreathing techniques.
Nitric Oxide (NO) has an affinity for hemoglobin about 400 times greater than carbon monoxide (it is generally an irreversible process since the end product is methemoglobin whereas hemoglobin’s binding with CO is more reversible) and for this reason it can also be used to measure diffusing capacity. DLNO can also be measured by single-breath, steady-state and rebreathing techniques. Because of its high affinity and the speed at which the binding of NO to hemoglobin occurs numerous researchers have assumed that DLNO is equivalent to DMNO (the membrane component of diffusing capacity). This is not really true, but it can be a useful fiction and in order to understand why it’s necessary to look at the basic physiology of diffusing capacity tests.
Roughton and Forster’s seminal 1957 paper showed that diffusion is the sum of two resistances. I’ve discussed this previously but specifically:
Where:
DMCO = membrane component
θCO = the rate at which CO binds to hemoglobin
Vc = pulmonary capillary blood volume
The first resistance (1/DMCO) is the resistance to the diffusion of CO through the alveolar-capillary membrane and blood plasma to the surface of the stagnant plasma boundary layer around a red blood cell. The second resistance refers to the diffusion rate of CO through the plasma boundary layer, then the wall and interior of the red blood cell and finally the rate of reaction with hemoglobin.
