To investigate whether hypercapnic acidosis protects against ventilator-induced lung injury (VILI) in vivo, we subjected 12 anesthetized, paralyzed rabbits to high tidal volume ventilation (25 cc/kg) at 32 breaths per minute and zero positive end-expiratory pressure for 4 hours. Each rabbit was randomized to receive either an FI(CO(2)) to achieve eucapnia (Pa(CO(2)) approximately 40 mm Hg; n = 6) or hypercapnic acidosis (Pa(CO(2)) 80-100 mm Hg; n = 6). Injury was assessed by measuring differences between the two groups' respiratory mechanics, gas exchange, wet:dry weight, bronchoalveolar lavage fluid protein concentration and cell count, and injury score. The eucapnic group showed significantly higher plateau pressures (27.0 +/- 2.5 versus 20.9 +/- 3.0; p = 0.016), change in Pa(O(2)) (165.2 +/- 19.4 versus 77.3 +/- 87.9 mm Hg; p = 0.02), wet:dry weight (9.7 +/- 2.3 versus 6.6 +/- 1.8; p = 0.04), bronchoalveolar lavage protein concentration (1,350 +/- 228 versus 656 +/- 511 micro g/ml; p = 0.03), cell count (6.86 x 10(5) +/- 0.18 x 10(5) versus 2.84 x 10(5) +/- 0.28 x 10(5) nucleated cells/ml; p = 0.021), and injury score (7.0 +/- 3.3 versus 0.7 +/- 0.9; p < 0.0001). We conclude that hypercapnic acidosis is protective against VILI in this model.

Hypoxic pulmonary vasoconstriction (HPV) serves to maintain optimal gas exchange by decreasing perfusion to hypoxic regions. However, global hypoxia and nonuniform HPV may result in overperfusion of poorly constricted regions leading to local edema seen in high-altitude pulmonary edema. To quantify the spatial distribution of HPV and its response to regional Po2 (Pr(O2)) among small lung regions, five pigs were anesthetized and mechanically ventilated in the supine posture. The animals were ventilated with an inspired O2 fraction (Fi(O2)) of 0.50 and 0.21 and then (in random order) 0.15, 0.12, and 0.09. Regional blood flow (Q) and alveolar ventilation (Va) were measured by using intravenous infusion of 15 microm and inhalation of 1-microm fluorescent microspheres, respectively. Pr(O2) was calculated for each piece at each Fi(O2). Lung pieces differed in their Q response to hypoxia in a manner related to their initial Va/Q with Fi(O2) = 0.21. Reducing Fi(O2) < 0.15 decreased Q to the initially high Va/Q (higher Pr(O2)) regions and forced Q into the low Va/Q (dorsal-caudal) regions. Resistance increased in most lung pieces as Pr(O2) decreased, reaching a maximum resistance when Pr(O2) is between 40 and 50 Torr. Local resistance decreased at PrO2 < 40 Torr. Pieces were statistically clustered with respect to their relative Q response pattern to each Fi(O2). Some clusters were shown to be spatially organized. We conclude that HPV is spatially heterogeneous. The heterogeneity of Q response may be related, in part, to the heterogeneity of baseline Va/Q.

We studied the spatial distribution of the abnormal ventilation-perfusion (Va/Q) units in a porcine model of acute pulmonary thromboembolism (APTE), using the fluorescent microsphere (FMS) technique. Four piglets ( approximately 22 kg) were anesthetized and ventilated with room air in the prone position. Each received approximately 20 g of preformed blood clots at time t = 0 min via a large-bore central venous catheter, until the mean pulmonary arterial pressure reached 2.5 times baseline. The distributions of regional Va and blood flow (Q) at five time points (t = -30, -5, 30, 60, 120 min) were mapped by FMS of 10 distinct colors, i.e., aerosolization of 1-mum FMS for labeling Va and intravenous injection of 15-mum FMS for labeling Q. Our results showed that, at t = 30 min following APTE, mean Va/Q (Va/Q = 2.48 +/- 1.12) and Va/Q heterogeneity (log SD Va/Q = 1.76 +/- 0.23) were significantly increased. There were also significant increases in physiological dead space (11.2 +/- 12.7% at 60 min), but the shunt fraction (Va/Q = 0) remained minimal. Cluster analyses showed that the low Va/Q units were mainly seen in the least embolized regions, whereas the high Va/Q units and dead space were found in the peripheral subpleural regions distal to the clots. At 60 and 120 min, there were modest recoveries in the hemodynamics and gas exchange toward baseline. Redistribution pattern was mostly seen in regional Q, whereas Va remained relatively unchanged. We concluded that the hypoxemia seen after APTE could be explained by the mechanical diversion of Q to the less embolized regions because of the vascular obstruction by clots elsewhere. These low Va/Q units created by high flow, rather than low Va, accounted for most of the resultant hypoxemia.

Hypoxic pulmonary vasoconstriction (HPV) is known to affect regional pulmonary blood flow distribution. It is unknown whether lungs with well-matched ventilation (V)/perfusion (Q) have regional differences in the HPV response. Five prone pigs were anesthetized and mechanically ventilated (positive end-expiratory pressure = 2 cmH2O). Two hypoxic preconditions [inspired oxygen fraction (FI(O2)) = 0.13] were completed to stabilize the animal's hypoxic response. Regional pulmonary blood Q and V distribution was determined at various FI(O2) (0.21, 0.15, 0.13, 0.11, 0.09) using the fluorescent microsphere technique. Q and V in the lungs were quantified within 2-cm3 lung pieces. Pieces were grouped, or clustered, based on the changes in blood flow when subjected to increasing hypoxia. Unique patterns of Q response to hypoxia were seen within and across animals. The three main patterns (clusters) showed little initial difference in V/Q matching at room air where the mean V/Q range was 0.92-1.06. The clusters were spatially located in cranial, central, and caudal portions of the lung. With decreasing FI(O2), blood flow shifted from the cranial to caudal regions. We determined that pulmonary blood flow changes, caused by HPV, produced distinct response patterns that were seen in similar regions across our prone porcine model.

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