Effect of increased alveolar surface tension on segmental pulmonary vascular resistance

The site of change in pulmonary vascular resistance (PVR) after surfactant displacement with the detergent diocytl sodium sulfosuccinate (OT) was studied in the isolated canine left lower lobe preparation. Changes in PVR were assessed using the arterial and venous occlusion technique and the vascular pressure-flow relationship. Changes in alveolar surface tension were confirmed from measurements of pulmonary compliance as well as from measurements of surface tension of extracts from lung homogenates. After surfactant depletion (the perfusion rate constant) the total pressure gradient (delta PT) across the lobe increased from 13.4 +/- 1 to 17.1 +/- 0.8 mmHg. This increase in delta PT was associated with a significant increase in the arterial and venous gradients (3.7 +/- 0.3 to 4.9 +/- 0.4 and 5.7 +/- 0.5 to 9.4 +/- 0.6 mmHg, respectively) and a decrease in middle pressure gradient (4.1 +/- 0.8 to 2.9 +/- 0.6 mmHg). The vascular pressure-flow relationship supported these findings and showed that the mean slope increased by 52% (P less than 0.05), whereas the pressure intercept decreased slightly but not significantly (3.7 +/- 0.7 to 3.2 +/- 0.8 mmHg). These results suggest that the resistance of arteries and veins increases, whereas the resistance of the middle segment decreases after surfactant depletion. These effects were apparently due to surface tension that acts directly on the capillary wall. Direct visualization of subpleural capillaries supported the notion that capillaries become distended and recruited as alveolar surface tension increases. In the normal lung (perfused at constant-flow rate) changes in alveolar pressure (Palv) were transmitted fully to the capillaries as suggested by equal changes in pulmonary arterial pressure.(ABSTRACT TRUNCATED AT 250 WORDS)     

Locus of hypoxic vasoconstriction in isolated ferret lungs

To determine whether hypoxic pulmonary vasoconstriction (HPV) occurs mainly in alveolar or extra-alveolar vessels in ferrets, we used two groups of isolated lungs perfused with autologous blood and a constant left atrial pressure (-5 Torr). In the first group, flow (Q) was held constant at 50, 100, and 150 ml.kg-1 X min-1, and changes in pulmonary arterial pressure (Ppa) were recorded as alveolar pressure (Palv) was lowered from 25 to 0 Torr during control [inspired partial pressure of O2 (PIO2) = 200 Torr] and hypoxic (PIO2 = 25 Torr) conditions. From these data, pressure-flow relationships were constructed at several levels of Palv. In the control state, lung inflation did not affect the slope of the pressure-flow relationships (delta Ppa/delta Q), but caused the extrapolated pressure-axis intercept (Ppa0), representing the mean backpressure to flow, to increase when Palv was greater than or equal to 5 Torr. Hypoxia increased delta Ppa/delta Q and Ppa0 at all levels of Palv. In contrast to its effects under control condition, lung inflation during hypoxia caused a progressive decrease in delta Ppa/delta Q, and did not alter Ppa0 until Palv was greater than or equal to 10 Torr. In the second group of experiments flow was maintained at 100 ml.kg-1 X min-1, and changes in lung blood volume (LBV) were recorded as Palv was varied between 20 and 0 Torr. In the control state, inflation increased LBV over the entire range of Palv. In the hypoxic state inflation decreased LBV until Palv reached 8 Torr; at Palv 8-20 Torr, inflation increased LBV.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

Effects of arterial ligation and embolization on pulmonary vascular pressure distribution

The effects of embolization on the longitudinal distribution of pulmonary vascular pressures with respect to vascular compliance were determined by the vascular inflow and outflow occlusion technique in isolated blood-perfused pig lungs treated with papaverine to prevent vasomotor responses. Embolization with microspheres having mean diameters of 75, 200, and 550 microns and with barrier beads (2 X 3 X 3.5 mm) significantly increased the pressure gradient across the relatively compliant middle region (delta Pm) without increasing the gradients across the relatively noncompliant regions on the arterial (delta Pa) or venous (delta Pv) ends of the vasculature. In contrast ligation of several lobar arteries caused delta Pa to increase from 0.9 +/- 0.3 to 5.9 +/- 1.1 mmHg but did not change delta Pm or delta Pv. Assuming that delta Pa and delta Pv measured by vascular occlusion result from cessation of flow through resistances, these data suggest that in isolated pig lungs the vessels at the boundary between the arterial and middle regions defined by the occlusion technique are arteries greater than 2-3 mm diam and smaller than lobar arteries.     

用显微穿刺技术直接测量微血管压力的伺服零方法研究

本实验制作了尖端的直径为０５－５０μｍ和斜面为２５°的玻璃微插管,成功地建立了用显微穿刺（ｍｉｃｒｏｐｕｎｃｔｕｒｅ）技术直接测量微血管压力（Ｐｍ）的伺服零方法（ｓｅｒｖｏｎｕｌｍｅｔｈｏｄ）,对自发高血压大鼠（ＳＨＲ）和正常血压大鼠（ＷＫＹ）肠系膜Ｐｍ进行了测量研究。结果表明,ＳＨＲ的平均动脉压（ＰＡ）和微动脉的Ｐｍ均明显大于ＷＫＹ的ＰＡ和Ｐｍ;ＰＡ在微动脉中明显降低,最大压降在直径小于５０μｍ的微动脉以及毛细血管中。     

Venous occlusion plethysmography reduces arterial diameter and flow velocity

The measurement of peripheral blood flow by plethysmography assumes that the cuff pressure required for venous occlusion does not decrease arterial inflow. However, studies in five normal subjects suggested that calf blood flow measured with a plethysmograph was less than arterial inflow calculated from Doppler velocity measurements. We hypothesized that the pressure required for venous occlusion may have decreased arterial velocity. Further studies revealed that systolic diameter of the superficial femoral artery under a thigh cuff decreased from 7.7 +/- 0.4 to 5.6 +/- 0.7 mm (P less than 0.05) when the inflation pressure was increased from 0 to 40 mmHg. Cuff inflation to 40 mmHg also reduced mean velocity 38% in the common femoral artery and 47% in the popliteal artery. Inflation of a cuff on the arm reduced mean velocity in the radial artery 22% at 20 mmHg, 26% at 40 mmHg, and 33% at 60 mmHg. We conclude that inflation of a cuff on an extremity to low pressures for venous occlusion also caused a reduction in arterial diameter and flow velocity.     

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.     

Effect of antigravity suit inflation on cardiovascular, PRA, and PVP responses in humans

Blood pressure, pulse rate (PR), serum osmolality and electrolytes, as well as plasma vasopressin (PVP) and plasma renin activity (PRA), were measured in five men and two women [mean age 38.6 +/- 3.9 (SE) yr] before, during, and after inflation of an antigravity suit that covered the legs and abdomen. After 24 h of fluid deprivation the subjects stood quietly for 3 h: the 1st h without inflation, the 2nd with inflation to 60 Torr, and the 3rd without inflation. A similar control noninflation experiment was conducted 10 mo after the inflation experiment using five of the seven subjects except that the suit was not inflated during the 3-h period. Mean arterial pressure increased by 14 +/- 4 (SE) Torr (P less than 0.05) with inflation and decreased by 15 +/- 5 Torr (P less than 0.05) after deflation. Pulse pressure (PP) increased by 7 +/- 2 Torr (P less than 0.05) with inflation and PR decreased by 11 +/- 5 beats/min (P less than 0.05); PP and PR returned to preinflation levels after deflation. Plasma volume decreased by 6.1 +/- 1.5% and 5.3 +/- 1.6% (P less than 0.05) during hours 1 and 3, respectively, and returned to base line during inflation. Inflation decreased PVP from 6.8 +/- 1.1 to 5.6 +/- 1.4 pg/ml (P less than 0.05) and abolished the significant rise in PRA during hour 1. Both PVP and PRA increased significantly after deflation: delta = 18.0 +/- 5.1 pg/ml and 4.34 +/- 1.71 ng angiotensin I X ml-1 X h-1, respectively. Serum osmolality and Na+ and K+ concentrations were unchanged during the 3 h of standing.(ABSTRACT TRUNCATED AT 250 WORDS)     

Effect of mean airway pressure on gas exchange during high-frequency oscillatory ventilation

We studied the effect of mean airway pressure (Paw) on gas exchange during high-frequency oscillatory ventilation in 14 adult rabbits before and after pulmonary saline lavage. Sinusoidal volume changes were delivered through a tracheostomy at 16 Hz, a tidal volume of 1 or 2 ml/kg, and inspired O2 fraction of 0.5. Arterial PO2 and PCO2 (PaO2, PaCO2), lung volume change, and venous admixture were measured at Paw from 5 to 25 cmH2O after either deflation from total lung capacity or inflation from relaxation volume (Vr). The rabbits were lavaged with saline until PaO2 was less than 70 Torr, and all measurements were repeated. Lung volume change was measured in a pressure plethysmograph. Raising Paw from 5 to 25 cmH2O increased lung volume by 48-50 ml above Vr in both healthy and lavaged rabbits. Before lavage, PaO2 was relatively insensitive to changes in Paw, but after lavage PaO2 increased with Paw from 42.8 +/- 7.8 to 137.3 +/- 18.3 (SE) Torr (P less than 0.001). PaCO2 was insensitive to Paw change before and after lavage. At each Paw after lavage, lung volume was larger, venous admixture smaller, and PaO2 higher after deflation from total lung capacity than after inflation from Vr. This study shows that the effect of increased Paw on PaO2 is mediated through an increase in lung volume. In saline-lavaged lungs, equal distending pressures do not necessarily imply equal lung volumes and thus do not imply equal PaO2.     

H2-receptor-mediated vasodilation contributes to postexercise hypotension.

The early (approximately 30 min) postexercise hypotension response after a session of aerobic exercise is due in part to H1-receptor-mediated vasodilation. The purpose of this study was to determine the potential contribution of H2-receptor-mediated vasodilation to postexercise hypotension. We studied 10 healthy normotensive men and women (ages 23.7 +/- 3.4 yr) before and through 90 min after a 60-min bout of cycling at 60% peak O2 uptake on randomized control and H2-receptor antagonist days (300 mg oral ranitidine). Arterial pressure (automated auscultation), cardiac output (acetylene washin) and femoral blood flow (Doppler ultrasound) were measured. Vascular conductance was calculated as flow/mean arterial pressure. Sixty minutes postexercise on the control day, femoral (delta62.3 +/- 15.6%, where Delta is change; P < 0.01) and systemic (delta13.8 +/- 5.3%; P = 0.01) vascular conductances were increased, whereas mean arterial pressure was reduced (Delta-6.7 +/- 1.1 mmHg; P < 0.01). Conversely, 60 min postexercise with ranitidine, femoral (delta9.4 +/- 9.2%; P = 0.34) and systemic (delta-2.8 +/- 4.8%; P = 0.35) vascular conductances were not elevated and mean arterial pressure was not reduced (delta-2.2 +/- 1.3 mmHg; P = 0.12). Furthermore, postexercise femoral and systemic vascular conductances were lower (P < 0.05) and mean arterial pressure was higher (P = 0.01) on the ranitidine day compared with control. Ingestion of ranitidine markedly reduces vasodilation after exercise and blunts postexercise hypotension, suggesting H2-receptor-mediated vasodilation contributes to postexercise hypotension.     

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.     

Relations among alveolar surface tension, surface area, volume, and recoil pressure

For pulmonary structure-function analysis excised rabbit lungs were fixed by vascular perfusion at six points on the pressure-volume (P-V) curve, i.e. at 40, 80, and 100% of total lung capacity (TLC) on inflation, at 80 and 40% TLC on deflation, and at 80% TLC on reinflation. Before fixation alveolar surface tensions (gamma) were measured in individual alveoli over the entire P-V loop, using an improved microdroplet method. A maximal gamma of approximately 30 mN/m was measured at TLC, which decreased during lung deflation to about 1 mN/m at 40% TLC. Surface tensions were considerably higher on the inflation limb starting from zero pressure than on the deflation limb (gamma-V hysteresis). In contrast, the corresponding alveolar surface area-volume (SA-V) relationship did not form a complete hysteresis over the entire volume range. There was a considerable difference in SA between lungs inflated to 40% TLC (1.49 +/- 0.11 m2) and lungs deflated to 40% TLC (2.19 +/- 0.21 m2), but at 80% TLC the values of SA were essentially the same regardless of the volume history. The data indicate that the gamma-SA hysteresis is only in part accountable for the P-V hysteresis and that the determinative factors of alveolar geometry change with lung volume. At low lung volumes airspace dimensions appear to be governed by an interplay between surface and tissue forces. At higher lung volumes the tissue forces become predominant.     

Cardiovascular responses to military antishock trouser inflation during standing arm exercise

Military antishock trousers (MAST) inflated to 50 mmHg were used with 12 healthy males (mean age 28 +/- 1 yr) to determine the effects of lower-body positive pressure on cardiac output (Q), stroke volume (SV), heart rate (HR), systolic blood pressure (SBP), diastolic blood pressure (DBP), mean arterial blood pressure (MABP), total peripheral resistance (TPR), and O2 uptake (VO2) during graded arm-cranking exercise. Subjects were studied while standing at rest and at 25, 50, and 75% of maximal arm-cranking VO2. At each level, rest or work was continued for 6 min with MAST inflated and for 6 min with MAST deflated. Order of inflation and deflation was alternated at each experimental rest or exercise level. Measurements were obtained during the last 2 min at each level. Repeated-measures analysis of variance revealed significant increases (P less than 0.001) in Q, SV, and MABP and a consistent decrease in HR with MAST inflation. There was no apparent change in Q/VO2 between inflated and control conditions. There was no effect of MAST inflation on VO2 or TPR. MAST inflation counteracts the gravitational effect of venous return in upright exercise, restoring central blood volume and thereby increasing Q and MABP from control. HR is decreased consequent to increased MABP through arterial baroreflexes. The associated decrease in TPR is not observed, being offset by the mechanical compression of leg vasculature with MAST inflation.     

Nature and distribution of vascular resistance in hypoxic pig lungs

We used the vascular occlusion technique in pig lungs isolated in situ to describe the effects of hypoxia on the distribution of vascular resistance and to determine whether the resistive elements defined by this technique behaved as ohmic or Starling resistors during changes in flow at constant outflow pressure, changes in outflow pressure at constant flow, and reversal of flow. During normoxia, the largest pressure gradient occurred across the middle compliant region of the vasculature (delta Pm). The major effect of hypoxia was to increase delta Pm and the gradient across the relatively noncompliant arterial region (delta Pa). The gradient across the noncompliant venous region (delta Pv) changed only slightly, if at all. Both delta Pa and delta Pv increased with flow but delta Pm decreased. The pressure at the arterial end of the middle region was independent of flow and, when outflow pressure was increased, did not increase until the outflow pressure of the middle region exceeded 8.9 Torr during normoxia and 18.8 Torr during hypoxia. Backward perfusion increased the total pressure gradient across the lung, mainly because of an increase in delta Pm. These results can be explained by a model in which the arterial and venous regions are represented by ohmic resistors and the middle region is represented by a Starling resistor in series and proximal to an ohmic resistor. In terms of this model, hypoxia exerted its major effects by increasing the critical pressure provided by the Starling resistor of the middle region and the ohmic resistance of the arterial region.     

Transmural pressure in rat initial subpleural lymphatics during spontaneous or mechanical ventilation

The role played by the mechanical tissue stress in supporting lymph formation and propulsion in thoracic tissues was studied in deeply anesthetized rats (n = 13) during spontaneous breathing or mechanical ventilation. After arterial and venous catheterization and insertion of an intratracheal cannula, fluorescent dextrans were injected intrapleurally to serve as lymphatic markers. After 2 h, the fluorescent intercostal lymphatics were identified, and the hydraulic pressure in lymphatic vessels (P lymph) and adjacent interstitial space (P int) was measured using micropuncture. During spontaneous breathing, end-expiratory P lymph and corresponding P int were -2.5 +/- 1.1 (SE) and 3.1 +/- 0.7 mmHg (P < 0.01), which dropped to -21.1 +/- 1.3 and -12.2 +/- 1.3 mmHg, respectively, at end inspiration. During mechanical ventilation with air at zero end-expiratory alveolar pressure, P lymph and P int were essentially unchanged at end expiration, but, at variance with spontaneous breathing, they increased at end inspiration to 28.1 +/- 7.9 and 28.2 +/- 6.3 mmHg, respectively. The hydraulic transmural pressure gradient (DeltaP tm = P lymph - P int) was in favor of lymph formation throughout the whole respiratory cycle (DeltaP tm = -6.8 +/- 1.2 mmHg) during spontaneous breathing but not during mechanical ventilation (DeltaP tm = -1.1 +/- 1.8 mmHg). Therefore, data suggest that local tissue stress associated with the active contraction of respiratory muscles is required to support an efficient lymphatic drainage from the thoracic tissues.     

Inflation of antishock trousers increases bronchial response to methacholine in healthy subjects

We studied changes in lung volumes and in bronchial response to methacholine chloride (MC) challenge when antishock trousers (AST) were inflated at venous occlusion pressure in healthy subjects in the standing posture, a maneuver known to shift blood toward lung vessels. On inflation of bladders isolated to lower limbs, lung volumes did not change but bronchial response to MC increased, as evidenced by a greater fall in the forced expiratory volume in 1 s (FEV1) at the highest dose of MC used compared with control without AST inflation (delta FEV1 = 0.94 +/- 0.40 vs. 0.66 +/- 0.46 liter, P less than 0.001). Full inflation of AST, i.e., lower limb and abdominal bladder inflated, significantly reduced vital capacity (P less than 0.001), functional residual capacity (P less than 0.01), and FEV1 (P less than 0.01) and enhanced the bronchial response to MC challenge compared with partial AST inflation (delta FEV1 = 1.28 +/- 0.47 liter, P less than 0.05). Because there was no significant reduction of lung volumes on partial AST inflation, the enhanced bronchial response to MC cannot be explained solely by changes in base-line lung volumes. An alternative explanation might be a congestion and/or edema of the airway wall on AST inflation. Therefore, to investigate further the mechanism of the increased bronchial response to MC, we pretreated the subjects with the inhaled alpha 1-adrenergic agonist methoxamine, which has both direct bronchoconstrictor and bronchial vasoconstrictor effects.(ABSTRACT TRUNCATED AT 250 WORDS)     

Leg intravenous pressure during head-up tilt

Leg vascular resistance is calculated as the arterial-venous pressure gradient divided by blood flow. During orthostatic challenges it is assumed that the hydrostatic pressure contributes equally to leg arterial, as well as to leg venous pressure. Because of venous valves, one may question whether, during orthostatic challenges, a continuous hydrostatic column is formed and if leg venous pressure is equal to the hydrostatic pressure. The purpose of this study was, therefore, to measure intravenous pressure in the great saphenous vein of 12 healthy individuals during 30 degrees and 70 degrees head-up tilt and compare this with the calculated hydrostatic pressure. The height difference between the heart and the right medial malleolus level represented the hydrostatic column. The results demonstrate that there were no differences between the measured intravenous pressure and the calculated hydrostatic pressure during 30 degrees (47.2 +/- 1.0 and 46.9 +/- 1.5 mmHg, respectively) and 70 degrees head-up tilt (83.9 +/- 0.9 and 85.1 +/- 1.2 mmHg, respectively). Steady-state levels of intravenous pressure were reached after 95 +/- 12 s during 30 degrees and 161 +/- 15 s during 70 degrees head-up tilt. In conclusion, the measured leg venous pressure is similar to the calculated hydrostatic pressure during orthostatic challenges. Therefore, the assumption that hydrostatic pressure contributes equally to leg arterial as well as to leg venous pressure during orthostatic challenges can be made.     

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.     

Effect of alveolar hypoxia on pulmonary fluid filtration in in situ dog lungs

We have studied the effect of alveolar hypoxia on fluid filtration characteristics of the pulmonary microcirculation in an in situ left upper lobe preparation with near static flow conditions (20 ml/min). In six dogs (group 1), rate of edema formation (delta W/delta t, where W is weight and t is time) was assessed over a wide range of vascular pressures under two inspired O2 fraction (FIO2) conditions (0.95 and 0.0 with 5% CO2-balance N2 in both cases). delta W/delta t was plotted against vascular pressure, and the best-fit linear regression was obtained. There was no significant difference (paired t test) in either threshold pressure for edema formation [18.3 +/- 1.8 and 17.1 +/- 1.2 (SE) mmHg, respectively] or the slopes (0.067 +/- 0.008 and 0.073 +/- 0.017 g.min-1. mmHg-1.100g-1, respectively). In another seven dogs (group 2), delta W/delta t was obtained at a constant vascular pressure of 40 mmHg under four FIO2 conditions (0.95, 0.21, 0.05, and 0.0, with 5% CO2-balance N2). Delta W/delta t for the four conditions averaged 0.60 +/- 0.11, 0.61 +/- 0.11, 0.61 +/- 0.10, and 0.61 +/- 0.10 (SE) g.min-1.mmHg-1.100g-1, respectively. No significant differences (ANOVA for repeated measures) were noted. We conclude that alveolar hypoxia does not alter the threshold for edema formation or delta W/delta t at a given microvascular pressure.