Effect of flow direction on collateral ventilation in excised dog lung lobes

We determined the effect of flow direction on the relationship between driving pressure and gas flow through a collaterally ventilating lung segment in excised cranial and caudal dog lung lobes. He, N2, and SF6 were passed through the lung segment distal to a catheter wedged in a peripheral airway. Gases were pushed through the segment by raising segment pressure (Ps) relative to airway opening pressure (Pao) and pulled from the segment by ventilating the lobe with the test gas, then lowering Ps relative to Pao. Driving pressures (Ps - Pao) between 0.25 and 2 cmH2O were evaluated at Pao values of 5, 10, and 15 cmH2O. Results were similar in cranial and caudal lobes. Flow increased as Ps - Pao increased and was greatest at Pao = 15 cmH2O for the least-dense gas (He). Although flow direction was not a significant first-order effect, there was significant interaction between volume, driving pressure, and flow direction. Dimensional analysis suggested that, although flow direction had no effect at Pao = 10 and 15 cmH2O, at Pao = 5 cmH2O, raising Ps relative to Pao increased the characteristic dimension of the flow pathways, and reducing Ps relative to Pao reduced the dimension. These data suggest that at large lobe volumes, airways (including collateral pathways) within the segment are maximally dilated and the stiffness of the parenchyma prevents any significant distortion when Ps is altered. At low lobe volumes, these pathways are affected by changes in transmural pressure due to the increased airway and parenchymal compliance.     

Effect of transpulmonary and driving pressures on collateral gas flow in dog lungs

The effect of changing segment pressure (Ps) and airway opening pressure (Pao) on flow through a collaterally ventilating lung segment was evaluated in intact and excised dog lungs. He, N2, and SF6 were passed through the lung segment distal to a catheter wedged in a peripheral airway at driving pressures (Ps - Pao) between 0.25 and 2 cm H2O. Eight excised caudal lobes were studied at Pao = 5, 10, and 15 cm H2O. Flow was directly related to Ps - Pao and Pao and inversely related to the density of the gas. A dimensionless plot of the driving pressure normalized to a reference dynamic pressure as a function of Reynolds number (Re) indicated that flow through the segment behaved as if it were laminar at Re less than 100 and that increasing Pao increased the dimension of the pathways conducting flow as shown previously. Small changes in Ps had no effect on pathway geometry or on the pattern of flow through the segment at Pao = 10 and 15 cmH2O. At Pao = 5 cm H2O increasing segment pressure appeared to increase the dimensions of the flow pathways slightly. Similar changes in Ps - Pao had no consistent effect on flow pattern or pathway geometry in six anesthetized, paralyzed, vagotomized dogs at functional residual capacity or after widely opening the chest (Pao = 5 cm H2O). These results suggest that, at large lobe volumes, airways (including collateral pathways) are maximally dilated and therefore relatively insensitive to small changes in segment pressure.(ABSTRACT TRUNCATED AT 250 WORDS)     

Effect of a regional increase in alveolar pressure on pulmonary blood flow.

We examined whether wedging a catheter (0.5 cm OD) into a subsegmental airway in dog (n = 6) or pig lungs (n = 5) and increasing pressure in the distal lung segment affected pulmonary blood flow. Dogs and pigs were anesthetized and studied in the prone position. Pulmonary blood flow was measured by injecting radiolabeled microspheres (15 microns diam) into the right atrium when airway pressure (Pao) was 0 cmH2O and pressure in the segment distal to the wedged catheter (Ps) was 0, 5, or 15 cmH2O and when Pao = Ps = 15 cmH2O. The lungs were excised, air-dried, and sectioned. Blood flow per gram dry weight normalized to cardiac output to the right or left lung, as appropriate, was calculated for the test segment, a control segment in the opposite lung corresponding anatomically to the test segment, the remainder of the lung containing the test segment (test lung), and the remainder of the lung containing the control segment (control lung). The presence of the catheter reduced blood flow in the test segment compared with that in the control segment and in the test lung. Blood flow was not affected by increasing pressure in the test segment. We conclude that, in studies designed to measure collateral ventilation in dog lungs, the presence of the wedged catheter is likely to have a greater effect on blood flow than the increase in pressure associated with measuring collateral airway resistance.     

Effects of maturation and aging on collateral ventilation in sheep

We studied collateral ventilation as a function of age by measuring the resistance (Rcoll) and time constant (Tcoll) of collateral airflow in young (2-10 mo), mature (16-24 mo), and old sheep (6-13 yr). Rcoll was 0.50 +/- 0.11 cmH2O X ml-1 X min (SE) in young sheep and decreased significantly to 0.05 +/- 0.02 and 0.02 +/- 0.01 cmH2O X ml-1 X min in mature and old sheep, respectively. Tcoll was 34.4 +/- 7.9 (SE) s in young sheep and decreased to 5.7 +/- 0.9 and 10.2 +/- 3.1 s in mature and old sheep, respectively. We conclude that a marked decrease in Rcoll and Tcoll occurs between birth and maturity but changes little with further aging. In the young an increased resistance and time constant of collateral airflow may accentuate ventilation perfusion imbalance and impair the removal of secretions in disease states.     

Cigarette smoke acutely increases collateral resistance in excised dog lobes

The acute effects of cigarette smoke or drug inhalation on collateral conductance (Gcoll) were studied in freshly excised dog lobes held at fixed volumes. A double-lumen catheter was wedged into a segmental bronchus, and air, smoke, or aerosol flowed into the blocked segment at a constant pressure of 2 cmH2O. A capsule glued over a small area of perforated pleura of the segment was used to measure alveolar pressure; the capsule could also be used to measure small airway flow (Vcap) through the segment. Gcoll was almost linearly dependent on lung volume, rising about fivefold between 20 and 100% inflation (30 cmH2O). During smoke inhalation Gcoll began decreasing almost immediately, roughly halving with the first cigarette and falling to about 20% after two cigarettes. Similar proportions were obtained at other lung volumes. Pulmonary conductance (oscillator) in the remainder of the lobe decreased only modestly to 78% of control after two cigarettes. In lobes exposed to 4.5% CO2 after air Gcoll rose 25-50%, but Vcap increased only 5-10%. However, acetylcholine chloride aerosol reduced both flows by similar ratios. Isoproterenol did not prevent or reverse smoke-induced collateral constriction but did reverse the effects of acetylcholine on both pathways. These results suggest that in excised lungs aerosols acted on larger segmental airways in series with collateral channels and with peripheral airways, whereas CO2 and particularly cigarette smoke provoked more marked effects on the most distal smooth muscle.     

Mechanical properties of small airways in excised pony lungs.

We evaluated the pressure-flow relationships in collaterally ventilating segments of excised pony lungs by infusing N2, He, Ne, or SF6 at known flows (V) through a catheter wedged in a peripheral airway. Measurements were made at segment- (Ps) to-airway opening (Pao) pressure differentials of 3-15 cmH2O when the lungs were held at transpulmonary pressures of 5, 10, and 15 cmH2O. The data were analyzed both by calculating collateral resistance (Ps-Pao/V) and by constructing Moody-type plots of normalized pressure drop [(Ps-Pao)/(1/2 rho U2, where rho is density and U is velocity)] against Reynolds number to assess the pattern of flow through the segment and the change in dimension of the flow channels as Ps and Pao were changed. The interpretations from these analyses were compared with radiographic measurements of the diameters of small airways within the collaterally ventilating lung segment at similar pressures. Collateral resistance increased as Ps-Pao increased at high Reynolds numbers, i.e., high flows or dense gas (SF6). Analysis of the Moody-type plots revealed that flow was density dependent at Reynolds number greater than 100, which frequently occurred when N2 was the inflow gas. The radiographic data revealed that small airway diameter increased as Ps-Pao increased at all lung volumes. In addition, at 5 cmH2O Pao, small-airway diameter was smaller for a given Ps in the nonhomogeneous case (Ps greater than Pao) than small-airway diameter for the same Ps in the homogeneous case (Ps = Pao). We interpret these data to suggest that the surrounding lung prevented the segment from expanding in the nonhomogeneous case.(ABSTRACT TRUNCATED AT 250 WORDS)     

Interstitial fibrosis and collateral ventilation

Interstitial fibrosis may increase resistance to collateral flow (Rcoll) because of decreased lung volume and destruction of collateral channels or it may decrease Rcoll because of emphysematous changes around fibrotic regions. In addition, if interstitial fibrosis involves a small region of lung periphery, interdependence from surrounding unaffected lung should produce relatively large changes in volume of the fibrotic region during lung inflation. We studied the effects of interstitial fibrosis on collateral airflow by measuring Rcoll at functional residual capacity (FRC) in nine mongrel dogs before and 28 days after the local instillation of bleomycin into selected lung segments. In six of these dogs Rcoll was also measured at a higher lung volume (transpulmonary pressure = 12 cmH2O above FRC pressure). Rcoll increased in fibrotic lung segments following local treatment with bleomycin. With lung inflation (high transpulmonary pressure) Rcoll fell a similar proportion in fibrotic and nonfibrotic lung regions. These observations suggest that collateral resistance increases in fibrotic segments because lung volume decreases or because collateral pathways are involved directly in the fibrotic process. Compensatory increases in collateral communications do not occur. In addition, pulmonary interdependence does not cause disproportionate increases in volume and decreases in Rcoll of the fibrotic region during lung inflation.     

Effects on body position and cholinergic blockade on mechanics of collateral ventilation

We studied the effects of position and cholinergic blockade on the mechanics of collateral ventilation in anesthetized paralyzed dogs. Resistance to collateral flow (Rcoll) is higher when an obstructed segment is dependent than when it is nondependent. Decreases of Rcoll in response to the local infusion of low oxygen mixtures are greater in dependent regions. We conclude that 1) changes in position affect Rcoll directly through local changes in lung volume related to the gradient of pleural pressure; 2) responses of collateral channels to local concentrations of CO2 and O2 are determined by ventilation perfusion relationships, which vary at different heights in the lung; and 3) resting cholinergic tone in the anesthetized dog varies at different heights in the lung.     

Hypocapnia does not alter collateral ventilation in sheep

Hypocapnic constriction has been proposed as a mechanism by which collateral pathways might rapidly alter ventilation to match perfusion. We studied the changes in response to hypocapnia with age in sheep, a species with collateral resistance (Rcoll) similar to those measured in humans. Measurements of Rcoll were made with either 5 or 10% CO2 and with air (hypocapnia) in 29 anesthetized sheep, ages 6 mo to 10 yr, with the wedged bronchoscope technique. Rcoll was 0.42 +/- 0.12, 0.58 +/- 0.18, 0.32 +/- 0.18, and 0.17 +/- 0.04 (SE) cmH2O.ml-1.min in 6-mo- and 1-, 2-, and 10-yr-old animals, respectively. These values were unchanged with hypocapnia. Despite the lack of a change in Rcoll with hypocapnia, administration of histamine aerosol (8 animals) through the bronchoscope increased Rcoll by 151 +/- 35% (P less than 0.05). These data suggest that although collateral pathways exist in sheep and are capable of constriction, they do not respond to hypocapnia. Furthermore, the response to hypocapnia is not influenced by age.     

Small airway pressure-diameter relationships during nonhomogeneous lung lobe inflation

The pressure-diameter behavior of airways within a collaterally ventilating segment of lung was evaluated radiographically in 12 excised dog lung lobes. The results were compared with the pressure-diameter behavior of airways in a lung region adjacent to the collaterally ventilating segment. Airways in each lung region were dusted with powdered tantalum, and airway diameters were measured during homogeneous and nonhomogeneous lobe inflation. Intrasegmental and extrasegmental airways behaved similarly during homogeneous lobe inflation; airway diameter increased as alveolar pressure increased. The lobe was inflated nonhomogeneously by raising pressure in the collaterally ventilating segment (Ps) while maintaining pressure at the lobar bronchus (Pao) constant at 5, 10, or 15 cmH2O. Increasing Ps at constant Pao reciprocally affected intrasegmental and extrasegmental airways. When Pao was low, intrasegmental airways were expanded, and extrasegmental airways were compressed when Ps was raised. When Pao was high, airway diameter was unaffected by increasing Ps presumably because the airways were already maximally expanded. A comparison of diameters during homogenous and nonhomogenous lobe inflation suggests a very small interdependence effect from the parenchyma surrounding the collaterally ventilating segment. These results demonstrate the combined effects of parenchymal properties and airway pressure-diameter relationships in determining the effect of local lung distortion on airway function.     

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)     

Parenchymal interdependence and airway response to methacholine in excised dog lobes

The objective of this investigation was to determine the minimum transpulmonary pressure (PL) at which the forces of interdependence between the airways and the lung parenchyma can prevent airway closure in response to maximal stimulation of the airways in excised canine lobes. We first present an analysis of the relationship between PL and the transmural pressure (Ptm) that airway smooth muscle must generate to close the airways. This analysis predicts that airway closure can occur at PL less than or equal to 10 cmH2O with maximal airway stimulation. We tested this prediction in eight excised canine lobes by nebulizing 50% methacholine into the airways while the lobe was held at constant PL values ranging from 25 to 5 cmH2O. Airway closure was assessed by comparing changes in alveolar pressure (measured by an alveolar capsule technique) and pressure at the airway opening during low-amplitude oscillations in lobar volume. Airway closure occurred in two of the eight lobes at PL = 10 cmH2O; in an additional five it occurred at PL = 7.5 cmH2O. We conclude that the forces of parenchymal interdependence per se are not sufficient to prevent airway closure at PL less than or equal to 7.5 cmH2O in excised canine lobes.     

Lung expansion and the perialveolar interstitial pressure gradient

We have determined the combined effects of lung expansion and increased extravascular lung water (EVLW) on the perialveolar interstitial pressure gradient. In the isolated perfused lobe of dog lung, we measured interstitial pressures by micropuncture at alveolar junctions (Pjct) and in adventitia of 30- to 50-microns microvessels (Padv) with stopped blood flow at vascular pressure of 3-5 cmH2O. We induced edema by raising vascular pressures. In nonedematous lobes (n = 6, EVLW = 3.1 +/- 0.3 g/g dry wt) at alveolar pressure of 7 cmH2O, Pjct averaged 0.5 +/- 0.8 (SD) cmH2O and the Pjct-Padv gradient averaged 0.9 +/- 0.5 cmH2O. After increase of alveolar pressure to 23 cmH2O the gradient was abolished in nonedematous lobes, did not change in moderately edematous lobes (n = 9, EVLW = 4.9 +/- 0.6 g/g dry wt), and increased in severely edematous lobes (n = 6, EVLW = 7.6 +/- 1.4 g/g dry wt). Perialveolar interstitial compliance decreased with increase of alveolar pressure. We conclude that increase of lung volume may reduce perialveolar interstitial liquid clearance by abolishing the Pjct-Padv gradient in nonedematous lungs and by compressing interstitial liquid channels in edematous lungs.     

Differential responses of tissue viscance and collateral resistance to histamine and leukotriene C4

Alterations in tissue viscance (Vti) and collateral resistance (Rcoll) are both used as indexes of peripheral lung responses. However, it is not known whether the two responses reflect the effects of activation of the same contractile elements. We measured differential responses in Vti and Rcoll to histamine and leukotriene (LT) C4 to determine whether each evoked a similar pattern of response. Using the wedged bronchoscope constant-flow technique, we measured Rcoll in lobar segments of anesthetized, paralyzed, open-chest, mechanically ventilated mongrel dogs. In addition, we measured (with an alveolar capsule) alveolar pressure (PA) within the segment under study. This allowed us to calculate Vti, the component of the PA change in phase with segment flow. Rcoll and Vti measurements were obtained under base-line conditions and after local delivery of aerosols generated from histamine and LTC4. In five out of five lobes studied with both histamine and LTC4, the fractional Rcoll response to histamine was greater than the fractional Rcoll response to LTC4. In contrast, in four out of five lobes examined, the fractional increase in Vti accompanying the histamine response was less than the fractional increase in Vti accompanying LTC4 administration. These data suggest that anatomically distinct contractile elements influence Vti and Rcoll insofar as LTC4 and histamine evoke quantitatively different changes in these two indexes of peripheral lung responses.     

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.     

Micropuncture measurement of alveolar liquid pressure in excised dog lung lobes

We have investigated the mechanism of alveolar liquid filling in pulmonary edema. We excised, degassed, and intrabronchially filled 14 dog lung lobes from nine dogs with 75, 150, 225, or 350 ml of 5% albumin solution, and then air inflated the lobes to a constant airway pressure of 25 cmH2O. By use of micropipettes, we punctured subpleural alveoli to measure alveolar liquid pressure by the servo-null technique. Alveolar liquid pressure was constant in all lobes despite differences in lobe liquid volume and averaged 10.6 +/- 1.3 cmH2O. Thus, in all lobes a constant pressure drop of 14.4 cmH2O existed from airway to alveolar liquid across the air-liquid interface. We attribute this finding, on the basis of the Laplace equation, to an air-liquid interface of constant radius in all the lobes. In fact, we calculated from the Laplace equation an air-liquid interface radius which equalled morphological estimates of alveolar radius. We conclude that in the steady state, alveoli that contained liquid have a constant radius of curvature of the air-liquid interface possibly because they are always completely liquid filled.     

Temporal and regional variability of collateral resistance response to histamine

Using the wedged bronchoscope technique, we measured the changes in collateral resistance (Rcoll) in dogs resulting from exposure to aerosols of increasing concentrations of histamine. Histamine dose-response curves were performed in each of two to three separate lobar segments of an individual mongrel dog's lungs. Five dogs were studied. The same segments were reexamined on later occasions (2-11 wk apart) to determine whether the responsiveness to histamine had altered with time. Measurements of base-line Rcoll for a given segment were reproducible (coefficient of variation 0.48). In contrast, we observed that the estimated dose of histamine required to increase Rcoll by 50% (ED150Rcoll) was extremely variable both among lung segments of an individual dog on a single experimental day (geometric mean variability of 40-fold) and for a given segment when reexamined on repeated occasions (geometric mean variability of 47-fold). The ED150Rcoll did not correlate with the base-line Rcoll. The degree of variability we observed suggests that peripheral contractile elements are under the influence of powerful local modulating factors that vary both regionally and temporally.     

Effect of dehydration on interstitial pressures in the isolated dog lung

We have determined the effect of dehydration on regional lung interstitial pressures. We stopped blood flow in the isolated blood-perfused lobe of dog lung at vascular pressure of approximately 4 cmH2O. Then we recorded interstitial pressures by micropuncture at alveolar junctions (Pjct), in perimicrovascular adventitia (Padv), and at the hilum (Phil). After base-line measurements, we ventilated the lobes with dry gas to decrease extravascular lung water content by 14 +/- 5%. In one group (n = 10), at constant inflation pressure of 7 cmH2O, Pjct was 0.2 +/- 0.8 and Padv was -1.5 +/- 0.6 cmH2O. After dehydration the pressures fell to -5.0 +/- 1.0 and -5.3 +/- 1.3 cmH2O, respectively (P less than 0.01), and the junction-to-advential gradient (Pjct-Padv) was abolished. In a second group (n = 6) a combination of dehydration and lung expansion with inflation pressure of 15 cmH2O further decreased Pjct and Padv to -7.3 +/- 0.7 and -7.1 +/- 0.7 cmH2O, respectively. Phil followed changes in Padv. Interstitial compliance was 0.6 at the junctions, 0.8 in adventitia, and 0.9 ml.cmH2O-1.100 g-1 wet lung at the hilum. We conclude, that perialveolar interstitial pressures may provide an important mechanism for prevention of lung dehydration.     

Interstitial fluid pressure gradient measured by micropuncture in excised dog lung

We have directly measured lung interstitial fluid pressure at sites of fluid filtration by micropuncturing excised left lower lobes of dog lung. We blood-perfused each lobe after cannulating its artery, vein, and bronchus to produce a desired amount of edema. Then, to stop further edema, we air-embolized the lobe. Holding the lobe at a constant airway pressure of 5 cmH2O, we measured interstitial fluid pressure using beveled glass micropipettes and the servo-null method. In 31 lobes, divided into 6 groups according to severity of edema, we micropunctured the subpleural interstitium in alveolar wall junctions, in adventitia around 50-micron venules, and in the hilum. In all groups an interstitial fluid pressure gradient existed from the junctions to the hilum. Junctional, adventitial, and hilar pressures, which were (relative to pleural pressure) 1.3 +/- 0.2, 0.3 +/- 0.5, and -1.8 +/- 0.2 cmH2O, respectively, in nonedematous lobes, rose with edema to plateau at 4.1 +/- 0.4, 2.0 +/- 0.2, and 0.4 +/- 0.3 cmH2O, respectively. We also measured junctional and adventitial pressures near the base and apex in each of 10 lobes. The pressures were identical, indicating no vertical interstitial fluid pressure gradient in uniformly expanded nonedematous lobes which lack a vertical pleural pressure gradient. In edematous lobes basal pressure exceeded apical but the pressure difference was entirely attributable to greater basal edema. We conclude that the presence of an alveolohilar gradient of lung interstitial fluid pressure, without a base-apex gradient, represents the mechanism for driving fluid flow from alveoli toward the hilum.     

Pressure-flow behavior of pulmonary interstitium

A method to measure the pressure-flow behavior of the interstitium around large pulmonary vessels is presented. Isolated rabbit lungs were degassed, and the air spaces and vasculature were inflated with a silicon rubber compound. After the rubber had hardened the caudal lobes were sliced into 1-cm-thick slabs. Two chambers were bonded to opposite sides of a slab enclosing a large blood vessel and were filled with saline containing 3 g/dl albumin. The flow through the interstitium surrounding the vessel was measured at a constant driving pressure of 5 cmH2O and at various mean interstitial pressures. Flow decreased with a reduction of mean interstitial pressure and reached a limiting minimum value at approximately -9 cmH2O. The pressure-flow behavior was analyzed under the assumptions that the interstitium is a porous material described by a single permeability constant that increases with hydration and that the expansion of the interstitium with interstitial pressure was due to the elastic response of the surrounding rubber compound. This resulted in an interstitial resistance (reciprocal of permeability constant) of 1.31 +/- 1.03 (SD) cmH2O.h.cm-2 and a ratio of interstitial cuff thickness to vessel radius of 0.022 +/- 0.007 (SD), n = 11. The phenomenon of flow limitation was demonstrated by holding the upstream pressure constant at 15 cmH2O and measuring the flow while the downstream pressure was reduced. The flow was limited at downstream pressures below -10 cmH2O.