Influence of lung volume and alveolar pressure on reverse pulmonary venous blood flow.

We have reported that left atrial blood refluxes through the pulmonary veins to gas-exchanging tissue after pulmonary artery ligation. This reverse pulmonary venous flow (Qrpv) was observed only when lung volume was changed by ventilation. This was believed to drive Qrpv by alternately distending and compressing the alveolar and extra-alveolar vessels. Because lung and pulmonary vascular compliances change with lung volume, we studied the effect of positive end-expiratory pressure (PEEP) on the magnitude of Qrpv during constant-volume ventilation. In prone anesthetized goats (n = 8), using the right lung to maintain normal blood gases, we ligated the pulmonary and bronchial arterial inflow to the left lung and ventilated each lung separately. A solution of SF6, an inert gas, was infused into the left atrium. SF6 clearance from the left lung was determined by the Fick principle at 0, 5, 10, and 15 and again at 0 cmH2O PEEP and was used to measure Qrpv. Left atrial pressure remained nearly constant at 20 cmH2O because the increasing levels of PEEP were applied to the left lung only. Qrpv was three- to fourfold greater at 10 and 15 than at 0 cmH2O PEEP. At these higher levels of PEEP, there were greater excursions in alveolar pressure for the same ventilatory volume. We believe that larger excursions in transpulmonary pressure during tidal ventilation at higher levels of PEEP, which compressed alveolar vessels, resulted in the reflux of greater volumes of left atrial blood, through relatively noncompliant extra-alveolar veins into alveolar corner vessels, and more compliant extra-alveolar arteries.     

Pulmonary vascular resistance after cessation of positive end-expiratory pressure

This report describes the pulmonary vascular response of infant lamb lung to abrupt cessation of positive end-expiratory pressure (PEEP) during volume-regulated continuous positive-pressure breathing (CPPB). In an intact, endobronchially ventilated preparation, the increase in left lung blood flow (QL) after abrupt cessation of 11 Torr left lung PEEP was found to be gradual, although peak airway pressure (Pmax) fell promptly from 36 to 14 Torr; 49% of the increase in QL occurred greater than 10 s after cessation of PEEP. Recruitment of zone I vasculature that had been created by balloon occlusion of the left pulmonary artery was found to occur promptly after balloon deflation. Isolated neonatal lamb lungs, perfused at constant flow rate, showed similar persistent elevation of pulmonary vascular resistance after cessation of 15 Torr PEEP, although Pmax fell abruptly from 39 to 12 Torr. This hysteresis was eliminated by calcium channel blockade with verapamil, and the magnitude of the change in pulmonary arterial pressure after either application or cessation of PEEP was reduced (25 and 26%, respectively). These observations suggest that, during CPPB, lung stretch alters neonatal pulmonary vascular tone or, by causing calcium channel-dependent lung volume hysteresis, modulates pulmonary vascular resistance. This interaction exaggerates the effect of airway pressure changes on pulmonary vascular resistance during mechanical ventilation.     

Longitudinal distribution of vascular compliance in the canine lung

With an isolated perfused canine lung, the compliance of pulmonary circulation was measured and partitioned into components corresponding to alveolar and extra-alveolar compartments. When the lungs were in zone 3, changes in outflow pressure (delta Po) affected all portions of the vasculature causing a change in lung blood volume (delta V). Thus the ratio delta V/delta Po in zone 3 represented the compliance of the entire pulmonary circulation (Cp) plus that of the left atrium (Cla). When the lungs were in zone 2, changes in Po affected only the extra-alveolar vessels that were downstream from the site of critical closure in the alveolar vessels. Thus the ratio delta V/delta Po with forward flow in zone 2 represented the compliance of the venous extra-alveolar vessels (Cv) plus Cla. With reverse flow in zone 2, delta V/delta Po represented the compliance of the arterial extra-alveolar vessels (Ca). The compliance of the alveolar compartment (Calv) was calculated from the difference between Cp and the sum of Ca + Cv. When Po was 6-11 mmHg, Cp was 0.393 +/- 0.0380 (SE) ml X mmHg-1 X kg-1 with forward perfusion and 0.263 +/- 0.0206 (SE) ml X mmHg-1 X kg-1 with reverse perfusion. Calv was 79 and 68% of Cp with forward and reverse perfusion, respectively. When Po was raised to 16-21 mmHg, Cp decreased to 0.225 +/- 0.0235 (SE) ml X mmHg-1 X kg-1 and 0.183 +/- 0.0133 (SE) ml X mmHg-1 X kg-1 with forward and reverse perfusion, respectively. Calv also decreased but remained the largest contributor to Cp. We conclude that the major site of pulmonary vascular compliance in the canine lung is the alveolar compartment, with minor contributions from the arterial and venous extra-alveolar segments.     

Marked differences between prone and supine sheep in effect of PEEP on perfusion distribution in zone II lung.

The classic four-zone model of lung blood flow distribution has been questioned. We asked whether the effect of positive end-expiratory pressure (PEEP) is different between the prone and supine position for lung tissue in the same zonal condition. Anesthetized and mechanically ventilated prone (n = 6) and supine (n = 5) sheep were studied at 0, 10, and 20 cm H2O PEEP. Perfusion was measured with intravenous infusion of radiolabeled 15-microm microspheres. The right lung was dried at total lung capacity and diced into pieces (approximately 1.5 cm3), keeping track of the spatial location of each piece. Radioactivity per unit weight was determined and normalized to the mean value for each condition and animal. In the supine posture, perfusion to nondependent lung regions decreased with little relative perfusion in nondependent horizontal lung planes at 10 and 20 cm H2O PEEP. In the prone position, the effect of PEEP was markedly different with substantial perfusion remaining in nondependent lung regions and even increasing in these regions with 20 cm H2O PEEP. Vertical blood flow gradients in zone II lung were large in supine, but surprisingly absent in prone, animals. Isogravitational perfusion heterogeneity was smaller in prone than in supine animals at all PEEP levels. Redistribution of pulmonary perfusion by PEEP ventilation in supine was largely as predicted by the zonal model in marked contrast to the findings in prone. The differences between postures in blood flow distribution within zone II strongly indicate that factors in addition to pulmonary arterial, venous, and alveolar pressure play important roles in determining perfusion distribution in the in situ lung. We suggest that regional variation in lung volume through the effect on vascular resistance is one such factor and that chest wall conformation and thoracic contents determine regional lung volume.     

Influence of vascular distending pressure on regional flows in isolated perfused dog lungs

To confirm the regional differences in vascular pressure vs. flow properties of lung regions that have been documented in zone 2 conditions [pulmonary venous pressure (Ppv) less than alveolar pressure], regional distending pressure vs. flow curves in zone 3 were generated by use of isolated blood-perfused dog lungs (3 right and 5 left lungs). Each lung was kept inflated at constant inflation pressure (approximately 50% of full inflation volume) while radioactively labeled microspheres were injected at different settings of Ppv. To achieve maximal vascular distension, Ppv was increased to approximately 30 cmH2O above alveolar pressure for the first injection. Subsequent injections were made at successively lower Ppv's. The difference between pulmonary arterial pressure and Ppv was kept constant for all injections. As was found in zone 2 conditions, there were differences in the regional distending pressure vs. flow curves among lung regions. To document the regional variability in the curves, the distribution of flow at a regional Ppv of 30 cmH2O above alveolar pressure was analyzed. There was a statistically significant linear gradient in this flow distribution from dorsal to ventral regions of the lungs but no consistent gradient in the caudad to cephalad direction. These results indicate that, even in near-maximally distended vessels, the dorsal regions of isolated perfused dog lungs have lower intrinsic vascular resistance compared with ventral regions.     

Influence of lung volume and left atrial pressure on reverse pulmonary venous blood flow

Infarction of the lung is uncommon even when both the pulmonary and the bronchial blood supplies are interrupted. We studied the possibility that a tidal reverse pulmonary venous flow is driven by the alternating distension and compression of alveolar and extra-alveolar vessels with the lung volume changes of breathing and also that a pulsatile reverse flow is caused by left atrial pressure transients. We infused SF6, a relatively insoluble inert gas, into the left atrium of anesthetized goats in which we had interrupted the left pulmonary artery and the bronchial circulation. SF6 was measured in the left lung exhalate as a reflection of the reverse pulmonary venous flow. No SF6 was exhaled when the pulmonary veins were occluded. SF6 was exhaled in increasing amounts as left atrial pressure, tidal volume, and ventilatory rates rose during mechanical ventilation. SF6 was not excreted when we increased left atrial pressure transients by causing mitral insufficiency in the absence of lung volume changes (continuous flow ventilation). Markers injected into the left atrial blood reached the alveolar capillaries. We conclude that reverse pulmonary venous flow is driven by tidal ventilation but not by left atrial pressure transients. It reaches the alveoli and could nourish the alveolar tissues when there is no inflow of arterial blood.     

Effect of lung inflation on lung blood volume and pulmonary venous flow

Phasic changes in lung blood volume (LBV) during the respiratory cycle may play an important role in the genesis of the respiratory wave in arterial pressure, or pulsus paradoxus. To better understand the effects of lung inflation on LBV, we studied the effect of changes in transpulmonary pressure (delta Ptp) on pulmonary venous flow (Qv) in eight isolated canine lungs with constant inflow. Inflation when the zone 2 condition was predominant resulted in transient decreases in Qv associated with increases in LBV. In contrast, inflation when the zone 3 condition was predominant resulted in transient increases in Qv associated with decreases in LBV. These findings are consistent with a model of the pulmonary vasculature that consists of alveolar and extra-alveolar vessels. Blood may be expelled from alveolar vessels but is retained in extra-alveolar vessels with each inflation. The net effect on LBV and thus on Qv is dependent on the zone conditions that predominate during inflation, with alveolar or extra-alveolar effects being greater when the zone 3 or zone 2 conditions predominate, respectively. Lung inflation may therefore result in either transiently augmented or diminished Qv. Phasic changes in left ventricular preload may therefore depend on the zone conditions of the lungs during the respiratory cycle. This may be an important modulator of respiratory variations in cardiac output and blood pressure.     

Hypoxia and angiotensin II infusion redistribute lung blood flow in lambs

To assess the effects of alveolar hypoxia and angiotensin II infusion on distribution of blood flow to the lung we performed perfusion lung scans on anesthetized mechanically ventilated lambs. Scans were obtained by injecting 1-2 mCi of technetium-labeled albumin macroaggregates as the lambs were ventilated with air, with 10-14% O2 in N2, or with air while receiving angiotensin II intravenously. We found that both alveolar hypoxia and infusion of angiotensin II increased pulmonary vascular resistance and redistributed blood flow from the mid and lower lung regions towards the upper posterior region of the lung. We assessed the effects of angiotensin II infusion on filtration pressure in six lambs by measuring the rate of lung lymph flow and the protein concentration of samples of lung lymph. We found that angiotensin II infusion increased pulmonary arterial pressure 50%, lung lymph flow 90%, and decreased the concentration of protein in lymph relative to plasma. These results are identical to those seen when filtration pressure increases during alveolar hypoxia. We conclude that alveolar hypoxia and angiotensin II infusion both increase fluid filtration in the lung by increasing filtration pressure. The increase in filtration pressure may be the result of a redistribution of blood flow in the lung with relative overperfusion of vessels in some areas and transmission of the elevated pulmonary arterial pressure to fluid-exchanging sites in those vessels.     

Acute increase in anastomotic bronchial blood flow after pulmonary arterial obstruction

We examined the acute changes in anastomotic bronchial blood flow (Qbr) serially for the 1st h after pulmonary arterial obstruction and subsequent reperfusion. We isolated and perfused the pulmonary circulation of the otherwise intact left lower lobe (LLL) with autologous blood in the widely opened chest of anesthetized dogs. Qbr was measured from the amount of blood overflowing from the closed pulmonary vascular circuit and the changes in the lobe weight. The right lung and the test lobe (LLL) were ventilated independently. The LLL, which was in zone 2 (mean pulmonary arterial pressure = 14.8 cm H2O, pulmonary venous pressure = 0, alveolar pressure = 5-15 cmH2O), was weighed continuously. The systemic blood pressure, gases, and acid-base status were kept constant. In control dogs without pulmonary arterial obstruction, the Qbr did not change for 2 h. Five minutes after pulmonary arterial obstruction, there was already a marked increase in Qbr, which then continued to increase for 1 h. After reperfusion, Qbr decreased. The increase in Qbr was greater after complete lobar than sublobar pulmonary arterial obstruction. It was unaltered when the downstream pulmonary venous pressure was increased to match the preobstruction pulmonary microvascular pressure. Thus, in zone 2, reduction in downstream pressure was not responsible for the increase in Qbr; neither was the decrease in alveolar PCO2, since ventilating the lobe with 10% CO2 instead of air did not change the Qbr. These findings suggest that there is an acute increase in Qbr after pulmonary arterial obstruction and that is not due to downstream pressure or local PCO2 changes.     

Lung microvascular pressure profile measured by micropuncture in anesthetized dogs

We have micropunctured the lung in the open thorax of 17 anesthetized dogs to measure microvascular pressure. After intravenous pentobarbital sodium (25 mg/kg), we exposed the left lung through a wide left thoracotomy, which required rib excision. Through a double-lumen endotracheal tube, we ventilated the right lung to maintain normal blood gases and pH while we held the left lung motionless at an inflation pressure of 5 cmH2O. To reduce motion on the surface of the left lower lobe, we resected the left upper lobe, placed a Plexiglas baffle between the lobe and the heart, and held the lobe surface in a suction ring. In accordance with procedures we have previously described, we micropunctured subpleural vessels to measure microvascular pressure. At base line when alveolar pressure exceeded left atrial pressure (zone 2 conditions), 21, 38, and 41% of the total pressure drop occurred, respectively, in the arterial, microvascular, and venous segments. When we raised left atrial pressure above alveolar pressure (zone 3 conditions), the corresponding pressure drops were 30, 55, and 20% of total. The blood flow in the superficial layer of the lung averaged 15% less than the flow in the deeper layers as measured by distribution of 99mTc-albumin macroaggregates. We conclude that the intact and the isolated lung preparations in dog exhibit similar distributions of subpleural microvascular pressure.     

Time-varying pulmonary arterial compliance

We tested the hypothesis that pulmonary arterial compliance (Ca) varies during the ventilatory cycle. Pressure and flow in the main pulmonary artery were measured in open-chest dogs under chloralose anesthesia (n = 12) with a positive-pressure volume-cycled ventilator. Input impedance was calculated from the pressure and flow waves of heart cycles obtained immediately after the start of inspiration (SI) and immediately after the start of expiration (SE). A lumped parameter model was used to calculate Ca from the input impedance spectrum of the main pulmonary artery. Three levels of positive end-expiratory pressure (PEEP) were used before and after meclofenamate (n = 6) or vagotomy (n = 6). Ca was significantly greater at SE than at SI at each level of PEEP. PEEP increased Ca at SE but not at SI. None of these changes was altered by meclofenamate or vagotomy, suggesting that these differences of Ca were due to passive mechanical effects rather than an active neurohumoral mechanisms. We conclude that Ca is time varying during the ventilatory cycle because it is altered by the dynamic increase of lung volume between SI and SE, but not with the quasi-static increase of lung volume induced by raising the level of PEEP. These changes of Ca were unaffected by vagal feedback or inhibition of cyclooxygenase. We suggest that the increased Ca just after the start of expiration may result from dynamic shifts of blood volume from the extra-alveolar to the alveolar vessels.     

Effect of thoracic duct drainage on hydrostatic pulmonary edema and pleural effusion in sheep

Positive end-expiratory pressure (PEEP) increases central venous pressure, which in turn impedes return of systemic and pulmonary lymph, thereby favoring formation of pulmonary edema with increased microvascular pressure. In these experiments we examined the effect of thoracic duct drainage on pulmonary edema and hydrothorax associated with PEEP and increased left atrial pressure in unanesthetized sheep. The sheep were connected via a tracheostomy to a ventilator that supplied 20 Torr PEEP. By inflation of a previously inserted intracardiac balloon, left atrial pressure was increased to 35 mmHg for 3 h. Pulmonary arterial, systemic arterial, and central venous pressure as well as thoracic duct lymph flow rate were continuously monitored, and the findings were compared with those in sheep without thoracic duct cannulation (controls). At the end of the experiment we determined the severity of pulmonary edema and the volume of pleural effusion. With PEEP and left atrial balloon insufflation, central venous and pulmonary arterial pressure were increased approximately threefold (P less than 0.05). In sheep with a thoracic duct fistula, pulmonary edema was less (extra-vascular fluid-to-blood-free dry weight ratio 4.8 +/- 1.0 vs. 6.1 +/- 1.0; P less than 0.05), and the volume of pleural effusion was reduced (2.0 +/- 2.9 vs. 11.3 +/- 9.6 ml; P less than 0.05). Our data signify that, in the presence of increased pulmonary microvascular pressure and PEEP, thoracic duct drainage reduces pulmonary edema and hydrothorax.     

Site of recruitment in the pulmonary microcirculation

Increasing the total surface area of the pulmonary blood-gas interface by capillary recruitment is an important factor in maintaining adequate oxygenation when metabolic demands increase. Capillaries are known to be recruited during conditions that raise pulmonary blood flow and pressure. To determine whether pulmonary arterioles and venules are part of the recruitment process, we made in vivo microscopic observations of the subpleural microcirculation (all vessels less than 100 microns) in the upper lung where blood flow is low (zone 2). To evoke recruitment, pulmonary arterial pressure was elevated either by an intravascular fluid load or by airway hypoxia. Of 209 arteriolar segments compared during low and high pulmonary arterial pressures, none recruited or derecruited. Elevated arterial pressure, however, did increase the number of perfused capillary segments by 96% with hypoxia and 165% with fluid load. Recruitment was essentially absent in venules (4 cases of recruitment in 289 segments as pressure was raised). These data support the concept that recruitment in the pulmonary circulation is exclusively a capillary event.     

Extra-alveolar veins are contiguous with, and leak fluid into, periarterial cuffs in rabbit lungs.

We previously observed physiological evidence that arterial and venous extra-alveolar vessels shared a common interstitial space. The purpose of the present investigation was to determine the site of this continuity to improve our understanding of interstitial fluid movement in the lung. Orange G and Evans blue dyes were added to the arterial and venous reservoirs, respectively, of excised rabbit lungs as they were placed 20 cmH2O into zone 1 (pulmonary arterial and venous pressures = 5 cmH2O, alveolar pressure = 25 cmH2O). After 10 s or 4 h the lungs were fixed by immersion in liquid N2, freeze-dried, cut into 5-mm serial slices, and examined by light macroscopy. Serial sections of 0.25-0.5 mm were subsequently examined by scanning electron microscopy. In the animals subjected to the zone 1 stress for 4 h, arterial and venous extra-alveolar vessels were surrounded by cuffs of edema. The edema ratio (cuff area divided by vessel lumen area) was greater around arteries than veins and decreased with increasing vessel size. Periarterial cuffs usually contained orange dye and frequently contained both orange and blue dye. Lymphatics containing orange or blue dye were frequently seen in periarterial cuffs. Scanning electron microscopy demonstrated that extra-alveolar veins of approximately 100 microns diameter were anatomically contiguous with arterial extra-alveolar vessel cuffs. In rabbit lungs, both arterial and venous extra-alveolar vessels (and/or alveolar corner vessels) leak fluid into perivascular cuffs surrounding arterial extra-alveolar vessels, and lymphatics located in the periarterial cuff contain fluid that originates from both the arterial and venous extra-alveolar vessels.     

Extra-alveolar vessel fluid filtration coefficients in excised and in situ canine lobes

We continuously weighed fully distended excised or in situ canine lobes to estimate the fluid filtration coefficient (Kf) of the arterial and venous extra-alveolar vessels compared with that of the entire pulmonary circulation. Alveolar pressure was held constant at 25 cmH2O after full inflation. In the in situ lobes, the bronchial circulation was interrupted by embolization. Kf was estimated by two methods (Drake and Goldberg). Extra-alveolar vessels were isolated from alveolar vessels by embolizing enough 37- to 74-micron polystyrene beads into the lobar artery or vein to completely stop flow. In excised lobes, Kf's of the entire pulmonary circulation by the Drake and Goldberg methods were 0.122 +/- 0.041 (mean +/- SD) and 0.210 +/- 0.080 ml X min-1 X mmHg-1 X 100 g lung-1, respectively. Embolization was not found to increase the Kf's. The mean Kf's of the arterial extra-alveolar vessels were 0.068 +/- 0.014 (Drake) and 0.069 +/- 0.014 (Goldberg) (24 and 33% of the Kf's for the total pulmonary circulation). The mean Kf's of the venous extra-alveolar vessels were similar [0.046 +/- 0.020 (Drake) and 0.065 +/- 0.036 (Goldberg) or 33 and 35% of the Kf's for the total circulation]. No significant difference was found between the extra-alveolar vessel Kf's of in situ vs. excised lobes. These results suggest that when alveolar pressure, lung volume, and pulmonary vascular pressures are high, approximately one-third of the total fluid filtration comes from each of the three compartments.     

Effects of PEEP on pulmonary hemodynamics in intact dogs with oleic acid pulmonary edema

The effects of positive end-expiratory pressure (PEEP) on the pulmonary circulation were studied in 14 intact anesthetized dogs with oleic acid (OA) lung injury. Transmural (tm) mean pulmonary arterial pressure (Ppa)/cardiac index (Q) plots with transmural left atrial pressure (Pla) kept constant were constructed in seven dogs, and Ppa(tm)/PEEP plots with Q and Pla(tm) kept constant were constructed in seven other dogs. Q was manipulated by using a femoral arteriovenous bypass and a balloon catheter inserted in the inferior vena cava. Pla was manipulated using a balloon catheter placed by thoracotomy in the left atrium. Ppa(tm)/Q plots were essentially linear. Before OA, the linearly extrapolated pressure intercept of the Ppa(tm)/Q relationship approximated Pla(tm). OA (0.09 ml/kg into the right atrium) produced a parallel shift of the Ppa(tm)/Q relationship to higher pressures; i.e., the extrapolated pressure intercept increased while the slope was not modified. After OA, 4 Torr PEEP (5.4 cmH2O) had no effect on the Ppa(tm)/Q relationship and 10 Torr PEEP (13.6 cmH2O) produced a slight, not significant, upward shift of this relationship. Changing PEEP from 0 to 12 Torr (16.3 cmH2O) at constant Q before OA led to an almost linear increase of Ppa(tm) from 14 +/- 1 to 19 +/- 1 mmHg. After OA, Ppa(tm) increased at 0 Torr PEEP but changing PEEP from 0 to 12 Torr did not significantly affect Ppa(tm), which increased from 19 +/- 1 to 20 +/- 1 mmHg. These data suggest that moderate levels of PEEP minimally aggravate the pulmonary hypertension secondary to OA lung injury.     

Air interface and elastic recoil affect vascular resistance in three zones of rabbit lungs

We examined the effect of the air interface on pulmonary vascular resistance (PVR) in zones 1, 2, and 3 by comparing pressure-flow data of air- and liquid-filled isolated rabbit lungs. Lungs were perfused with Tyrode's solution osmotically balanced with 1% albumin and 4% dextran and containing the vasodilator papaverine (0.05 mg/ml). Lung volume was varied by negative pleural pressure form 0 to -25 cmH2O. Pulmonary artery (Ppa) and venous (Ppv) pressures were fixed at various levels relative to the lung base. Alveolar pressure (PA) was always zero, and perfusate flow was measured continuously. In zone 1 Ppa was -2.5 cmH2O and Ppv was -15 cmH2O. In zone 2 Ppa was 10 cmH2O and Ppv was -5 cmH2O. In zone 3 Ppa was 15 cmH2O and Ppv was 8 cmH2O. We found that in zone 1 the interface was essential for perfusion, but in zones 2 and 3 it had much lesser effects. In general, PVR depended almost uniquely (i.e., with small hysteresis) on transpulmonary pressure, whereas a large hysteresis existed between PVR and lung volume. PVR was high in collapsed and especially in atelectatic lungs, fell sharply with moderate inflation, and within the ranges of vascular pressure studied did not rise again toward total lung capacity. These results suggest that in zone 1 the interface maintains the patency of some alveolar vessels, probably in corners. The majority of alveolar septal vessels appears to be exposed directly to PA in zones 2 and 3, because at equal transpulmonary pressure the PVR is similar in the presence or absence of an interface.     

Alveolar vessel behavior in the zone 2 lung inferred from indicator-dilution data

To gain insight into the changes occurring in alveolar vessels when alveolar pressure exceeds venous pressure at the downstream end of the alveolar vessels (zone 2), we compared the uptake of serotonin and the extravascular volume accessible to 3HOH (Qev) under zone 2 and 3 conditions in isolated dog lung lobes. We also examined the influence of occluding some of the small pulmonary arteries with 58- to 548-micron-diam beads on the serotonin uptake and Qev. We found that, with the bead embolization, both the serotonin uptake and the Qev were reduced, whereas the change from zone 3 to 2 reduced serotonin uptake but did not change Qev. A plausible explanation for these observations is that the beads occluded vessels that were relatively large compared with those in which significant transvascular 3HOH exchange and serotonin uptake take place. Perfusion ceased in the collection of capillaries normally served by the obstructed arteries. Thus the extravascular water and the serotonin uptake sites downstream from the obstructions were not accessible to the indicators during the short time interval of the indicator passage through the lung. On the other hand, the change from zone 3 to zone 2 resulted in the collapse of small individual capillary segments within the alveolar vessel bed. Since the serotonin does not readily diffuse from the vessels through the tissue, it could not reach the endothelial cells of the collapsed capillaries. However, since the distances for diffusion between collapsed capillaries and neighboring perfused capillaries were small, the more highly diffusible 3HOH had access to the same Qev under both zone 2 and 3 conditions.(ABSTRACT TRUNCATED AT 250 WORDS)     

Pulmonary vascular resistance in the fluorocarbon-filled lung

Pulmonary vascular resistance was investigated in the fluorocarbon-filled lung in an in situ isolated lung preparation. Lungs were perfused at constant flow (100 ml X min-1 X kg-1) with whole blood from a donor cat. left atrial pressure was held constant at zero pressure. Measurements of pulmonary arterial pressure enabled calculation of pulmonary vascular resistance. Regional changes in pulmonary blood flow were determined by the microsphere technique. During quasi-static deflation over a range of 0-30 mmHg, dependent alveolar pressure was consistently greater for a volume of fluorocarbon than for gas, with each pressure-volume curve for the fluorocarbon-filled lung shifted to the right of the curve for the gas-filled lung. In turn, pulmonary vascular resistance was found to increase linearly as a function of increasing alveolar pressure, independent of the medium in the lung. Thus, for a given volume, pulmonary vascular resistance was consistently greater in the fluorocarbon-filled lung compared with the gas-filled lung. This increase in pulmonary vascular resistance was accompanied by a redistribution of pulmonary blood flow in which blood flow to the dependent region was decreased in the fluorocarbon-filled lung compared with the gas-filled lung. Conversely, the less-dependent regions of the lung received a relatively greater percentage of blood flow when filled with fluorocarbon compared with gas. These findings suggest that pulmonary vascular resistance is increased during liquid ventilation, largely as the result of mechanical interaction at the alveolar-vascular interface.