The functional dependence between tracheal gas exchange and tracheal b
lood flow has been previously reported using six inert gases (sulfur h
exafluoride, ethane, cyclopropane, halothane, ether, and acetone) in a
unidirectionally ventilated (1 ml/s) canine trachea (J. E. Souders, S
. C. George, N. L. Polissar, E. R. Swenson, and M. P. Hlastala. J. App
l. Physiol. 79: 918-928, 1995). To understand the relative contributio
n of perfusion-, diffusion- and ventilation-related resistances to air
way gas exchange, a dynamic model of the bronchial circulation has bee
n developed and added to the existing structure of a previously descri
bed model (S. C. George, A. L. Babb, and M. P. Hlastala. J. Appl. Phys
iol. 75: 2439-2449, 1993). The diffusing capacity of the trachea (in m
l gas . s(-1) . atm(-1)) was used to optimize the fit of the model to
the experimental data. The experimental diffusing capacities as predic
ted by the model in a 10-cm length of trachea are as follows: sulfur h
exafluoride, 0.000055; ethane, 0.00070; cyclopropane, 0.0046; halothan
e, 0.029; ether, 0.10; and acetone, 1.0. The diffusing capacities are
reduced relative to an estimated diffusing capacity. The ratio of expe
rimental to estimated diffusing capacity ranges from 4 to 23%. The mod
el predicts that over the ventilation-to-tracheal blood flow range (10
-700) attained experimentally, tracheal gas exchange is limited primar
ily by perfusion- and diffusion-related resistances. However, the cont
ribution of the ventilation-related resistance increases with increasi
ng gas solubility and cannot be neglected in the case of acetone. The
increased role of diffusion in tracheal gas exchange contrasts with pe
rfusion-limited alveolar exchange and is due primarily to the increase
d thickness of the bronchial mucosa.