In the mammalian lung, alveolar gas and blood are separated by an extremely thin membrane, despite the fact that mechanical failure could be catastrophic for gas exchange. We raised the pulmonary capillary pressure in anesthetized rabbits until stress failure occurred. At capillary transmural pressures greater than or equal to 40 mmHg, disruption of the capillary endothelium and alveolar epithelium was seen in some locations. The three principal forces acting on the capillary wall were analyzed. 1) Circumferential wall tension caused by the transmural pressure. This is approximately 25 dyn/cm (25 mN/m) at failure where the radius of curvature of the capillary is 5 microns. This tension is small, being comparable with the tension in the alveolar wall associated with lung elastic recoil. 2) Surface tension of the alveolar lining layer. This contributes support to the capillaries that bulge into the alveolar spaces at these high pressures. When protein leakage into the alveolar spaces occurs because of stress failure, the increase in surface tension caused by surfactant inhibition could be a powerful force preventing further failure. 3) Tension of the tissue elements in the alveolar wall associated with lung inflation. This may be negligible at normal lung volumes but considerable at high volumes. Whereas circumferential wall tension is low, capillary wall stress at failure is very high at approximately 8 x 10(5) dyn/cm2 (8 x 10(4) N/m2) where the thickness is only 0.3 microns. This is approximately the same as the wall stress of the normal aorta, which is predominantly composed of collagen and elastin. The strength of the thin part of the capillary wall is probably attributable to the collagen IV of the basement membranes. The safety factor is apparently small when the capillary pressure is raised during heavy exercise. Stress failure causes increased permeability with protein leakage, or frank hemorrhage, and probably has a role in several types of lung disease.
We used multiple-breath N2 washouts (MBNW) to study the inhomogeneity of ventilation in four normal humans (mean age 42.5 yr) before, during, and after 9 days of exposure to microgravity on Spacelab Life Sciences-1. Subjects performed 20-breath MBNW at tidal volumes of approximately 700 ml and 12-breath MBNW at tidal volumes of approximately 1,250 ml. Six indexes of ventilatory inhomogeneity were derived from data from 1) distribution of specific ventilation (SV) from mixed-expired and 2) end-tidal N2, 3) change of slope of N2 washout (semilog plot) with time, 4) change of slope of normalized phase III of successive breaths, 5) anatomic dead space, and 6) Bohr dead space. Significant ventilatory inhomogeneity was seen in the standing position at normal gravity (1 G). When we compared standing 1 G with microgravity, the distributions of SV became slightly narrower, but the difference was not significant. Also, there were no significant changes in the change of slope of the N2 washout, change of normalized phase III slopes, or the anatomic and Bohr dead spaces. By contrast, transition from the standing to supine position in 1 G resulted in significantly broader distributions of SV (P < 0.05) and significantly greater changes in the changes in slope of the N2 washouts (P < 0.001), indicating more ventilatory inhomogeneity in that posture. Thus these techniques can detect relatively small changes in ventilatory inhomogeneity. We conclude that the primary determinants of ventilatory inhomogeneity during tidal breathing in the upright posture are not gravitational in origin.
To test the hypothesis that maximal O2 uptake (VO2max) can be limited by O2 diffusion in the peripheral tissue, we kept O2 delivery [blood flow X arterial O2 content (CaO2)] to maximally contracting muscle equal between 1) low flow-high CaO2 and 2) high flow-low CaO2 conditions. The hypothesis predicts, because of differences in the capillary PO2 profile, that the former condition will result in both a higher VO2max and muscle effluent venous PO2 (PVO2). We studied the relations among VO2max, PVO2, and O2 delivery during maximal isometric contractions in isolated, in situ dog gastrocnemius muscle (n = 6) during these two conditions. O2 delivery was matched by varying arterial O2 partial pressure and adjusting flow to the muscle accordingly. A total of 18 matched O2 delivery pairs were obtained. As planned, O2 delivery was not significantly different between the two treatments. In contrast, VO2max was significantly higher [10.4 +/- 0.5 (SE) ml.100 g-1.min-1; P = 0.01], as was PVO2 (25 +/- 1 Torr; P less than 0.01) in the low flow-high CaO2 treatment compared with the high flow-low CaO2 treatment (9.1 +/- 0.4 ml.100 g-1.min-1 and 20 +/- 1 Torr, respectively). The rate of fatigue was greater in the high flow-low CaO2 condition, as was lactate output from the muscle and muscle lactate concentration. The results of this study show that VO2max is not uniquely dependent on O2 delivery and support the hypothesis that VO2max can be limited by peripheral tissue O2 diffusion.
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