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.     

Measurement of bronchial arterial blood flow and bronchovascular resistance in sheep

We studied the bronchial arterial blood flow (Qbr) and bronchial vascular resistance (BVR) in sheep prepared with carotid-bronchial artery shunt. Nine adult sheep were anesthetized, and through a left thoracotomy a heparinized Teflon-tipped Silastic catheter was introduced into the bronchial artery. The other end of the catheter was brought out through the chest wall and through a neck incision was introduced into the carotid artery. A reservoir filled with warm heparinized blood was connected to this shunt. The height of blood column in the reservoir was kept constant at 150 cm by adding more blood. Qbr was measured, after interrupting the carotid-bronchial artery flow, by the changes in the reservoir volume. The bronchial arterial back pressure (Pbr) was measured through the shunt when both carotid-bronchial artery and reservoir Qbr had been temporarily interrupted. The mean Qbr was 34.1 +/- 2.9 (SE) ml/min, Pbr = 17.5 +/- 3.3 cmH2O, BVR = 3.9 +/- 0.5 cmH2O X ml-1 X min, mean pulmonary arterial pressure = 21.5 +/- 3.6 cmH2O, and pulmonary capillary wedge pressure (Ppcw) = 14.3 +/- 3.7 cmH2O. We further studied the effect of increased left atrial pressure on these parameters by inflating a balloon in the left atrium. The left atrial balloon inflation increased Ppcw to 25.3 +/- 3.1 cmH2O, Qbr decreased to 21.8 +/- 2.4 ml/min (P less than 0.05), and BVR increased to 5.5 +/- 1.0 cmH2O.ml-1.min (P less than 0.05).(ABSTRACT TRUNCATED AT 250 WORDS)     

Temperature alters bronchial blood flow response to pulmonary arterial obstruction

Lobar bronchial blood flow has been reported to increase and decrease acutely after pulmonary arterial obstruction (PAO). Because bronchial blood flow (Qbr) to the trachea and bronchi is influenced by inspired air temperature, we investigated whether temperature differences could explain these disparate results. In 10 open-chested dogs the left lower lobe (LLL) was isolated and perfused in situ with autologous blood at a controlled temperature with an independent vascular circuit. The abdomen and the chest of the dog were enclosed in a Plexiglas box in which air was fully humidified and temperature could be regulated. Qbr, determined by the reference flow technique using 16 micron microspheres, was measured before and 30 min after onset of PAO with the air in the box being either at 27 or 39 degrees C and with warmed LLL blood (37 degrees C) in the latter condition. Anastomotic bronchial blood flow [Qbr(s-p), determined as overflow from the closed LLL vascular circuit and measured in ml X min-1 X 100 g dry lung wt-1 X 100 Torr mean systemic pressure-1] was measured continuously at both temperatures. Both before and after PAO, Qbr and Qbr(s-p) were closely correlated: Qbr (ml/min) = 1.12 + 0.978Qbr(s-p); R = 0.912. This was true regardless of the presence or the absence of pulmonary flow, showing that the distribution of bronchial blood flow between the anastomotic and the nonanastomotic portion does not change acutely during PAO. When the air in the box was 27 degrees C, Qbr(s-p) was 19.5 +/- 5.2 (SE) and increased to 38.6 +/- 8.1 with PAO (P less than 0.007).(ABSTRACT TRUNCATED AT 250 WORDS)     

Zone 2 and zone 3 pulmonary blood flow

In the West model of zonal distribution of pulmonary blood flow, increases in flow down zone 2 are attributed to an increase in driving pressure and a decrease in resistance resulting from recruitment and distension. The increase in flow down zone 3 is attributed to a decrease in resistance only. Recent studies indicate that, besides the pressure required to maintain flow through a vessel, there is an added pressure cost that must be overcome in order to initiate flow. These additional pressure costs are designated critical pressures (Pcrit). Because Pcrit exceed alveolar pressure, the distinction between zones in the West model becomes less secure, and the explanation for the increase in flow even in West zone 3 requires reexamination. We used two methods to test the hypothesis that the Pcrit is the pertinent backpressure to flow even in zone 3, when the pulmonary venous pressure (Ppv) exceeds alveolar pressure (PA) but is less than Pcrit in the isolated canine left caudal lobe. First, PA was maintained at 5 cmH2O, and pressure flow (P-Q) characteristics were obtained in zone 2 and zone 3. Next, with PA still at 5 cmH2O, we maintained a constant flow and measured the change in pulmonary arterial pressure as Ppv was varied. Both techniques indicated that the pertinent backpressure to flow was the greater of either Pcrit or Ppv and that PA was never the pertinent backpressure to flow. Also, our results indicate no significant change in the geometry of the flow channels between zone 2 and zone 3. These findings refine the zonal model of the pulmonary circulation.     

Bronchial collateral vessel micropuncture pressure in postobstructive pulmonary vasculopathy.

Postobstructive pulmonary vasculopathy, produced by chronic ligation of one pulmonary artery, markedly increases bronchial blood flow. Previously, using arterial and venous occlusion, we determined that bronchial collaterals enter the pulmonary circuit at the distal end of the arterial segment. In this study, we tested the hypothesis that pressure in bronchial collaterals (Pbr) closely approximates that at the downstream end of the arterial segment (Pao). We pump perfused [111 +/- 10 (SE) ml/min] left lower lobes of seven open-chest live dogs 3-15 mo after ligation of the left main pulmonary artery. Bronchial blood flow was 122 +/- 16 ml/min. We measured pulmonary arterial and venous pressures and, by arterial and venous occlusion, respectively, Pao and the pressure at the upstream end of the venous segment (Pvo). Pbr was obtained by micropuncture of 34 pleural surface bronchial vessels 201 +/- 16 microns in diameter. We found that Pbr (14.4 +/- 1.0 mmHg) was similar to Pao (15.0 +/- 0.8 mmHg) but differed significantly (P < 0.01) from Pvo (11.3 +/- 0.5 mmHg). In addition, Pbr was independent of systemic arterial pressure and bronchial vessel diameter. Light and electron microscopy revealed that, in the lobes with the ligated pulmonary artery, the new bronchial collaterals entered the thickened pleura from the parenchyma via either bronchovascular bundles or interlobular septa and had sparsely muscularized walls. We conclude that, in postobstructive pulmonary vasculopathy, bronchial collateral pressure measured by micropuncture is very close to the pressure in precapillary pulmonary arteries and that most of the pressure drop in the bronchial collaterals occurs in vessels > 350 microns in diameter.     

Acute increases in anastomotic bronchial systemic to pulmonary blood flow due to generalized lung injury

Since pulmonary blood flow to regions involved in adult respiratory disease syndrome (ARDS) is reduced by hypoxic vasoconstriction, compression by cuffs of edema, and local thromboses, we postulated that the bronchial circulation must enlarge to provide for the inflammatory response. We measured anastomotic bronchial systemic to pulmonary blood flow [QBr(s-p)] serially in a lung lobe in 31 open-chest dogs following a generalized lobar injury simulating ARDS. The pulmonary circulation of the weighed left lower lobe (LLL) was isolated and perfused (zone 2) with autologous blood in anesthetized dogs. QBr(s-p) was measured from the amount of blood which overflowed from this closed vascular circuit corrected by any changes in the lobe weight. The LLL was ventilated with 5% CO2 in air. The systemic blood pressure (volume infusion), gases, and acid-base status (right lung ventilation) were kept constant. We injured the LLL via the airway by instilling either 0.1 N HCl or a mixture of glucose and glucose oxidase or via the pulmonary vessels by injecting either alpha-naphthylthiourea or oleic acid into the LLL pulmonary artery. In both types of injury, there was a prompt rise in QBr(s-p) (mean rise = 247% compared with control), which was sustained for the 2 h of observation. The cause of this increase in flow was studied. Control instillation of normal saline into the airways or into the pulmonary vessels did not change QBr(s-p) nor did a similar increase in lobar fluid (weight) due to hydrostatic edema. Neither cardiac output nor systemic blood pressure increased.(ABSTRACT TRUNCATED AT 250 WORDS)     

Flow characteristics of open vessels in zone 1 rabbit lungs

To describe the flow characteristics of vessels open in zone 1, we perfused isolated rabbit lungs with Tyrode's solution containing 1% albumin, 4% dextran, and papaverine (0.05 mg/ml). Lungs were expanded by negative pleural pressure (Ppl) of -10, -15, -20, and -25 cmH2O. Pulmonary arterial (Ppa) and venous (Ppv) pressures were varied relative to alveolar pressure (PA = 0) and measured 5-10 mm inside the pleura (i) and outside (o) of the lungs. With Ppa(o) at -2.5 cmH2O, we constructed pressure-flow (P-Q) curves at each Ppl by lowering Ppv(o) until Q reached a maximum, indicating fully developed zone 1 choke flow. Maximum flows were negligible until Ppl fell below -10 cmH2O, then increased rapidly at Ppl of -15 and -20 cmH2O, and at Ppl of -25 cmH2O reached about 15 ml.min-1.kg body wt-1. The Ppv(o) at which flow became nearly constant depended on degree of lung inflation and was 5-8 cmH2O more positive than Ppl. As Ppv(o) was lowered below Ppa(o), Ppv(i) remained equal to Ppv(o) until Ppv(i) became fixed at a pressure 2-3 cmH2O more positive than Ppl. At this point the choke flow was therefore located in veins near the pleural boundary. No evidence of choke flow (only ohmic resistance) was seen in the intrapulmonary segment of the vessels remaining open in zone 1. With Ppv(o) held roughly at Ppl, Q could be stopped by lowering Ppa(o), at which time Ppa(i) was several cmH2O above Ppv(i), showing that intrapulmonary vessel closure had occurred.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

Continuity of arterial and venous extra-alveolar interstitium in excised rabbit lungs

We studied the interdependence of arterial and venous extra-alveolar vessel (EAV) leakage on the rate of pulmonary vascular fluid filtration (measured as the change in lung weight over time). Edema was produced in continually weighed, excised rabbit lungs kept in zone 1 (alveolar pressure = 25 cmH2O) by increasing pulmonary arterial (Ppa) and/or venous (Ppv) pressure from 5 to 20 cmH2O (relative to the lung base) and continuing this hydrostatic stress for 3-5 h. Raising Ppa and Ppv simultaneously produced a lower filtration rate than the sum of the filtration rates obtained when Ppa and Ppv were raised separately, while the lung gained from 20 to 95% of its initial weight. When vascular pressure was elevated in either EAV segment, fluid filtration always decreased rapidly as the lung gained up to 30-45% of its initial weight. Filtration then decreased more slowly. The lungs became isogravimetric at 60 and 85% weight gain when the Ppa or Ppv was elevated, respectively; when Ppa and Ppv were raised simultaneously substantial fluid filtration continued even after 140% weight gain. We conclude that the arterial and venous EAV's share a common interstitium in the zone 1 condition, this interstitium cannot be represented as a single compartment with a fixed resistance and compliance, and arterial and venous EAV leakage influences leakage from the other segment.     

Venous occlusion pressure and vascular permeability in the dog lung after air embolization

Pulmonary edema has frequently been associated with air embolization of the lung. In the present study the hemodynamic effects of air emboli (AE) were studied in the isolated mechanically ventilated canine right lower lung lobe (RLL), pump perfused at a constant blood flow. Air was infused via the pulmonary artery (n = 7) at 0.6 ml/min until pulmonary arterial pressure (Pa) rose 250%. While Pa rose from 12.4 +/- 0.6 to 44.6 +/- 2.0 (SE) cmH2O (P less than 0.05), venous occlusion pressure remained constant (7.0 +/- 0.5 to 6.8 +/- 0.6 cmH2O; P greater than 0.05). Lobar vascular resistance (RT) increased from 2.8 +/- 0.3 to 12.1 +/- 0.2 Torr.ml-1.min.10(-2) (P less than 0.05), whereas the venous occlusion technique used to determine the segmental distribution of vascular resistance indicated the increase in RT was confined to vessels upstream to the veins. Control lobes (n = 7) administered saline at a similar rate showed no significant hemodynamic changes. As an index of microvascular injury the pulmonary filtration coefficient (Kf) was obtained by sequential elevations of lobar vascular pressures. The Kf was 0.11 +/- 0.01 and 0.07 +/- 0.01 ml.min-1.Torr-1.100 g RLL-1 in AE and control lobes, respectively (P less than 0.05). Despite a higher Kf in AE lobes, total lobe weight gains did not differ and airway fluid was not seen in the AE group. Although air embolization caused an increase in upstream resistance and vascular permeability, venous occlusion pressure did not increase, and marked edema did not occur.     

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.     

Pulmonary hemodynamics and lung water content during splanchnic ischemic shock

Pulmonary hemodynamics and lung water content were evaluated in open-chest dogs during splanchnic arterial occlusion (SAO) shock. Mean pulmonary arterial pressure [Ppa = 13.0 +/- 0.6 (SE) mmHg] and pulmonary venous pressure (4.1 +/- 0.2 mmHg) were measured by direct cannulation and the capillary pressure (Ppc = 9.0 +/- 0.6 mmHg) estimated by the double-occlusion technique. SAO shock did not produce a significant change in Ppa or Ppc despite a 90% decrease in cardiac output. An 18-fold increase in pulmonary vascular resistance occurred, and most of this increase (70%) was on the venous side of the circulation. No differences in lung water content between shocked and sham-operated dogs were observed. The effect of SAO shock was further evaluated in the isolated canine left lower lobe (LLL) perfused at constant flow and outflow pressure. The addition of venous blood from shock dogs to the LLL perfusion circuit caused a transient (10-15 min) increase in LLL arterial pressure (51%) that could be reversed rapidly with papaverine. In this preparation, shock blood produced either a predominantly arterioconstriction or a predominantly venoconstriction. These results indicate that both arterial and venous vasoactive agents are released during SAO shock. The consistently observed venoconstriction in the intact shocked lung suggests that other factors, in addition to circulating vasoactive agents, contribute to the pulmonary hemodynamic response of the open-chest shocked dog.     

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.     

The effect of closing the ductus arteriosus on the pulmonary circulation of the fetal sheep

In the mammalian fetus the ductus arteriosus allows right ventricular output to be shunted away from the lungs to the systemic circulation. This study was performed to determine how closing the ductus arteriosus of the fetal sheep would affect the pulmonary circulation. Under halothane anaesthesia 6 near-term fetal sheep were delivered with the umbilical circulation intact. Catheters were placed in the right atrium, the pulmonary artery, and the aorta. Pulmonary blood flow was measured by injecting radioactive microspheres into the right atrium while a reference sample was withdrawn from the pulmonary artery. Closing the ductus arteriosus increased pulmonary arterial pressure by 22% from 51 +/- 3 to 62 +/- 3 mmHg and increased pulmonary blood flow disproportionately by 198% from 232 +/- 74 to 692 +/- 80 ml/min per 100g. Thus, pulmonary vascular resistance decreased by 75% from 0.451 +/- 0.65 to 0.095 +/- 0.010 mmHg 100g min/ml. These findings extend the observation that pressure and flow in the pulmonary circulation of the air-breathing lung do not have a linear relationship passing through the origin to include a striking example in the fluid-filled lung of the intact fetus. They also raise questions about the nature of the elevated vascular resistance in the fetal lung.     

Effect of hypoxia on bronchial circulation

We studied the effect of systemic hypoxia on the bronchial vascular pressure-flow relationship in anesthetized ventilated sheep. The bronchial artery, a branch of the bronchoesophageal artery, was cannulated and perfused with a pump with blood from a femoral artery. Bronchial blood flow was set so bronchial arterial pressure approximated systemic arterial pressure. For the group of 25 sheep, control bronchial blood flow was 22 ml/min or 0.7 ml.min-1.kg-1. During the hypoxic exposure, animals were ventilated with a mixture of N2 and air to achieve an arterial PO2 (PaO2) of 30 or 45 Torr. For the more severe hypoxic challenge, bronchial vascular resistance (BVR), as determined by the slope of the linearized pressure-flow curve, decreased acutely from 3.8 +/- 0.4 mmHg.ml-1.min to 2.9 +/- 0.3 mmHg.ml-1.min after 5 min of hypoxia. However, this vasodilation was not sustained, and BVR measured at 30 min of hypoxia was 4.2 +/- 0.8 mmHg.ml-1.min. The zero flow intercept, an index of downstream pressure, remained unaltered during the hypoxic exposure. Under conditions of moderate hypoxia (PaO2 = 45 Torr), BVR decreased from 4.6 +/- 0.3 to 3.8 +/- 0.4 mmHg.ml-1.min at 5 min and remained dilated at 30 min (3.6 +/- 0.5 mmHg.ml-1.min). To determine whether dilator prostaglandins were responsible for the initial bronchial vascular dilation under conditions of severe hypoxia (PaO2 approximately equal to 30 Torr), we studied an additional group of animals with pretreatment with the cyclooxygenase inhibitors indomethacin (2 mg/kg) and ibuprofen (12.5 mg/kg).(ABSTRACT TRUNCATED AT 250 WORDS)     

Systemic blood flow to sheep lung: comparison of flow probes and microspheres.

Discrepancies exist between experimental measurements of the systemic blood flow to sheep lung by use of microsphere techniques and flow probes on the bronchial artery. In these studies, we simultaneously measured the blood flow through the bronchial artery, using a transit time flow probe, and the systemic blood flow to left lung, using radioactive microspheres. All measurements were made on conscious sheep previously prepared with chronic catheterizations of the left atrium, aorta, and vena cava and a flow probe around the bronchial artery. Inflatable occluder cuffs were placed around the pulmonary and bronchoesophageal arteries. Bronchial artery blood flow in six sheep was 25.3 +/- 5.2 ml/min or 0.4% of the cardiac output. Systemic blood flow to left lung, measured with microspheres, was 54.1 +/- 14.2 ml/min. Calculated systemic blood flow to that portion of sheep lung perfused by the bronchial artery was 127.6 +/- 35.3 ml/min or 1.9% of cardiac output. Occlusion of the bronchoesophageal artery reduced bronchial artery flow to near zero, whereas total systemic blood to the lung was reduced by only 55%. Blood flow to the intraparenchymal cartilaginous airways was reduced 60-90% after occlusion of the bronchoesophageal artery. Sheep, like most mammals, have multiple and complex systemic arterial inputs to the lungs. We conclude that multiple branches of the bronchoesophageal artery provide most but not all of the systemic blood flow to the intraparenchymal cartilaginous airways but that over one-half of the total systemic blood flow to sheep lung comes from sources other than the common bronchial artery.     

Effects of airway pressure on bronchial blood flow

We studied the effects of increased airway pressure caused by increasing levels of positive end-expiratory pressure (PEEP) on bronchial arterial pressure-flow relationships. In eight alpha-chloralose-anesthetized mechanically ventilated sheep (23-27 kg), the common bronchial artery, the bronchial branch of the bronchoesophageal artery, was cannulated and perfused with a pump. The control bronchial blood flow (avg 12 +/- 1 ml/min or 0.48 ml X min-1 X kg-1) was set to maintain mean bronchial arterial pressure equal to systemic blood pressure. Pressure-flow curves of the bronchial circulation were measured by making step changes in bronchial blood flow, and changes in these curves were analyzed with measurements of the pressure at zero flow and the slope of the linearized curve. The zero-flow pressure represents the effective downstream pressure, and the slope represents the resistance through the bronchial vasculature. At a constant bronchial arterial pressure of 100 mmHg, an 8 mmHg increase in mean airway pressure caused a 40% reduction in bronchial blood flow. Under constant flow conditions, increases in mean airway pressure with the application of PEEP caused substantial increases in bronchial arterial pressure, averaging 4.6 mmHg for every millimeters of mercury increase in mean airway pressure. However, bronchial arterial pressure at zero flow increased approximately one-for-one with increases in mean airway pressure. Thus the acute sensitivity of the bronchial artery to changes in mean airway pressure results primarily from changes in bronchovascular resistance and not downstream pressure.     

Pulmonary vascular responsiveness in cold-exposed calves

The pulmonary vascular responses to acute hypoxia and to infusions of histamine and 5-hydroxytryptamine (5-HT) were recorded in unanesthetized standing bull calves under neutral (16-18 degrees C) and cold (3-5 degrees C) temperature conditions. Cold exposure alone resulted in a significant increase in pulmonary arterial wedge pressure from 10.2 +/- 3.5 to 15.9 +/- 4.9 Torr (1 Torr = 133.322 Pa). Resistance to blood flow between the pulmonary wedge and the left atrium significantly increased from 0.50 +/- 0.51 to 1.21 +/- 0.78 mmHg . L-1 . min-1 (1 mmHg = 133.322 Pa) with cold exposure. This apparent pulmonary venoconstrictor response to cold exposure was further evaluated to determine if hypoxia, histamine, or 5-HT responsiveness was altered by cold exposure. Twelve minutes of hypoxia increased pulmonary arterial and systemic arterial pressures, heart rate, and respiratory rate similarly in cold and neutral temperatures. Cold exposure did not alter the dose-related reductions of systemic arterial and pulmonary arterial pressures in response to histamine. Similarly, the decreases in systemic arterial pressure and heart rate and increases in pulmonary arterial and left atrial pressures in response to 5-HT were not significantly different in cold and neutral conditions. It was concluded that acute, mild cold exposure results in an increase in resistance to blood flow in the pulmonary venous circulation without a general increase in pulmonary vascular reactivity, as measured by responses to hypoxia, histamine, and 5-HT.     

Development of pulmonary intravascular macrophage function in newborn lambs.

We sought to determine whether pulmonary intravascular macrophages are involved in pulmonary vascular sensitivity to intravenously injected particles in sheep. We estimated that newborn lambs have few of these macrophages at birth but develop a 10-fold greater density within 2 wk. Awake, chronically instrumented newborn lambs showed no change in pulmonary vascular driving pressure (pulmonary arterial minus left atrial pressure) after injection of either liposomes [2 +/- 3 (SD) cmH2O; n = 5] or Monastral blue particles (3 +/- 2 cmH2O; n = 6) and showed no net pulmonary production of thromboxane B2, the stable metabolite of the vasoconstrictor thromboxane A2. In contrast, five of those lambs 2 wk later showed both an increase in pulmonary vascular driving pressure after injection of liposomes and Monastral blue (20 +/- 16 and 25 +/- 15 cmH2O, respectively; P < 0.05) and net pulmonary production of thromboxane B2 (171 +/- 103 and 429 +/- 419 pg/ml plasma, respectively; P < 0.05). Older lambs (n = 5) had higher pulmonary uptakes than newborn lambs (n = 6) of radioactive liposomes (47 +/- 13 vs. 12 +/- 10%; P < 0.01) and Monastral blue (53 +/- 6 vs. 21 +/- 10%; P < 0.05). We conclude that pulmonary intravascular macrophages are responsible for the sensitivity of sheep to intravenous foreign particles and are essential for a cascade of processes leading to microvascular injury.