Factors That Affect the Rate of
Gas Diffusion Through the Respiratory Membrane
Referring to the earlier discussion of diffusion of gases in water,
one can apply the same principles and math-ematical formulas to diffusion of
gases through the respiratory membrane. Thus, the factors that deter-mine how
rapidly a gas will pass through the mem-brane are (1) the thickness of the membrane, (2) the surface area of the membrane, (3) the diffusion coeffi-cient of the gas in the substance of the
membrane, and (4) the partial pressure
difference of the gas between the two sides of the membrane.
The thickness of the
respiratory membrane occa-sionally increases—for instance, as a result of
edema fluid in the interstitial space of the membrane and in the alveoli—so
that the respiratory gases must then diffuse not only through the membrane but
also through this fluid. Also, some pulmonary diseases cause fibrosis of the
lungs, which can increase the thickness of some portions of the respiratory
mem-brane. Because the rate of diffusion through the mem-brane is inversely
proportional to the thickness of the membrane, any factor that increases the
thickness to more than two to three times normal can interfere sig-nificantly
with normal respiratory exchange of gases.
The surface area of the
respiratory membrane can be greatly decreased by many conditions. For
instance, removal of an entire lung decreases the total surface area to one
half normal. Also, in emphysema, many
of the alveoli coalesce, with dissolution of many alveolar walls. Therefore,
the new alveolar chambers are much larger than the original alveoli, but the
total surface area of the respiratory membrane is often decreased as much as
fivefold because of loss of the alveolar walls. When the total surface area is
decreased to about one third to one fourth normal, exchange of gases through
the membrane is impeded to a signifi-cant degree, even under resting conditions, and during competitive sports and
other strenuous exercise, even the slightest decrease in surface area of the
lungs can be a serious detriment to respiratory exchange of gases.
The diffusion coefficient
for transfer of each gas through the respiratory membrane depends on the gas’s solubility in the membrane and, inversely,
on the square root of the gas’s molecular weight. The rateof diffusion
in the respiratory membrane is almost exactly the same as that in water, for
reasons explained earlier. Therefore, for a given pressure difference, carbon
dioxide diffuses about 20 times as rapidly as oxygen. Oxygen diffuses about
twice as rapidly as nitrogen.
The pressure difference
across the respiratory mem-brane is the difference between the partial pressure
of the gas in the alveoli and the partial pressure of the gas in the pulmonary
capillary blood. The partial pres-sure represents a measure of the total number
of mol-ecules of a particular gas striking a unit area of the alveolar surface
of the membrane in unit time, and the pressure of the gas in the blood
represents the number of molecules that attempt to escape from the blood in the
opposite direction. Therefore, the difference between these two pressures is a
measure of the nettendency for the
gas molecules to move through themembrane. When the partial pressure of a gas in
the alveoli is greater than the pressure of the gas in the blood, as is true
for oxygen, net diffusion from the alveoli into the blood occurs; when the
pressure of the gas in the blood is greater than the partial pressure in the
alveoli, as is true for carbon dioxide, net diffusion from the blood into the
alveoli occurs.
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