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To facilitate computational toxicology, we developed an approach for generating high-resolution lung-anatomy and particle-deposition mouse models. Major processing steps of our method include mouse preparation, serial block-face cryomicrotome imaging, and highly automated image analysis for generating three-dimensional (3D) mesh-based models and volume-based models of lung anatomy (airways, lobes, sublobes, and near-acini structures) that are linked to local particle-deposition measurements. Analysis resulted in 34 mouse models covering 4 different mouse strains (B6C3F1: 8, BALB/C: 11, C57Bl/6: 8, and CD-1: 7) as well as both sexes (16 male and 18 female) and different particle sizes [2 μm ( n = 15), 1 μm ( n = 16), and 0.5 μm ( n = 3)]. On average, resulting mouse airway models had 1,616.9 ± 298.1 segments, a centerline length of 597.6 ± 59.8 mm, and 1,968.9 ± 296.3 outlet regions. In addition to 3D geometric lung models, matching detailed relative particle-deposition measurements are provided. All data sets are available online in the lapdMouse archive for download. The presented approach enables linking relative particle deposition to anatomical structures like airways. This will in turn improve the understanding of site-specific airflows and how they affect drug, environmental, or biological aerosol deposition. NEW & NOTEWORTHY Computer simulations of particle deposition in mouse lungs play an important role in computational toxicology. Until now, a limiting factor was the lack of high-resolution mouse lung models and measured local particle-deposition information, which are required for developing accurate modeling approaches (e.g., computational fluid dynamics). With the developed imaging and analysis approach, we address this issue and provide all of the raw and processed data in a publicly accessible repository.

Despite substantial development of sophisticated subject-specific computational models of aerosol transport and deposition in human lungs, experimental validation of predictions from these new models is sparse. We collected aerosol retention and exhalation profiles in seven healthy volunteers and six subjects with mild-to-moderate COPD (FEV1=50–80%predicted) in the supine posture. Total deposition was measured during continuous breathing of 1 and 2.9 µm-diameter particles (tidal volume of 1 L, flow rate of 0.3 L/s and 0.75 L/s). Bolus inhalations of 1 µm particles were performed to penetration volumes of 200, 500 and 800 mL (flow rate of 0.5 L/s). Aerosol bolus dispersion (H), deposition, and mode shift (MS) were calculated from these data. There was no significant difference in total deposition between healthy subjects and those with COPD. Total deposition increased with increasing particle size and also with increasing flow rate. Similarly, there was no significant difference in aerosol bolus deposition between subject groups. Yet, the rate of increase in dispersion and of decrease in MS with increasing penetration volume was higher in subjects with COPD than in healthy volunteers (H: 0.798±0.205 vs. 0.527±0.122 mL/mL, p=0.01; MS: −0.271±0.129 vs. −0.145 ±0.076 mL/mL, p=0.05) indicating larger ventilation inhomogeneities (based on H) and increased flow sequencing (based on MS) in the COPD than in the healthy group. In conclusion, in the supine posture, deposition appears to lack sensitivity for assessing the effect of lung morphology and/or ventilation distribution alteration induced by mild-to-moderate lung disease on the fate of inhaled aerosols. However, other parameters such as aerosol bolus dispersion and mode shift may be more sensitive parameters for evaluating models of lungs with moderate disease.

Computer models for inhalation toxicology and drug-aerosol delivery studies rely on ventilation pattern inputs for predictions of particle deposition and vapor uptake. However, changes in lung mechanics due to disease can impact airflow dynamics and model results. It has been demonstrated that non-invasive, in vivo, 4DCT imaging (3D imaging at multiple time points in the breathing cycle) can be used to map heterogeneities in ventilation patterns under healthy and disease conditions. The purpose of this study was to validate ventilation patterns measured from CT imaging by exposing the same rats to an aerosol of fluorescent microspheres (FMS) and examining particle deposition patterns using cryomicrotome imaging.Six male Sprague-Dawley rats were intratracheally instilled with elastase to a single lobe to induce a heterogeneous disease. After four weeks, rats were imaged over the breathing cycle by CT then immediately exposed to an aerosol of ∼ 1 μm FMS for ∼ 5 minutes. After the exposure, the lungs were excised and prepared for cryomicrotome imaging, where a 3D image of FMS deposition was acquired using serial sectioning. Cryomicrotome images were spatially registered to match the live CT images to facilitate direct quantitative comparisons of FMS signal intensity with the CT-based ventilation maps.Comparisons of fractional ventilation in contiguous, non-overlapping, 3D regions between CT-based ventilation maps and FMS images showed strong correlations in fractional ventilation (r = 0.888, p0.0001).We conclude that ventilation maps derived from CT imaging are predictive of the 1 μm aerosol deposition used in ventilation-perfusion heterogeneity inhalation studies.

A highly automated method for the segmentation of airways in the serial block-face cryomicrotome images of rat lungs is presented. First, a point inside of the trachea is manually specified. Then, a set of candidate airway centerline points is automatically identified. By utilizing a novel path extraction method, a centerline path between the root of the airway tree and each point in the set of candidate centerline points is obtained. Local disturbances are robustly handled by a novel path extraction approach, which avoids the shortcut problem of standard minimum cost path algorithms. The union of all centerline paths is utilized to generate an initial airway tree structure, and a pruning algorithm is applied to automatically remove erroneous subtrees or branches. Finally, a surface segmentation method is used to obtain the airway lumen. The method was validated on five image volumes of Sprague-Dawley rats. Based on an expert-generated independent standard, an assessment of airway identification and lumen segmentation performance was conducted. The average of airway detection sensitivity was 87.4% with a 95% confidence interval (CI) of (84.9, 88.6)%. A plot of sensitivity as a function of airway radius is provided. The combined estimate of airway detection specificity was 100% with a 95% CI of (99.4, 100)%. The average number and diameter of terminal airway branches was 1179 and 159 μm, respectively. Segmentation results include airways up to 31 generations. The regression intercept and slope of airway radius measurements derived from final segmentations were estimated to be 7.22 μm and 1.005, respectively. The developed approach enables the quantitative studies of physiology and lung diseases in rats, requiring detailed geometric airway models.

We aimed to investigate the role of endothelin-mediated vasoconstriction following acute pulmonary thromboembolism (APTE). Thirteen anesthetized piglets (~25 kg) were ventilated with 0 PEEP. Cardiac output (Qt) and wedge pressure (Pw) were measured by a Swan Ganz catheter, along with arterial and venous blood gases. APTE was induced by autologous blood clots (~0.8 g/kg, 12-16 pieces) via a jugular venous catheter at time = 0 minutes until the mean pulmonary arterial pressure (Ppa) was about 2.5 times the baseline at 30 minutes. Eight control animals (Group 1) received only normal saline afterward, while the remaining five (Group 2) received at time = 40-minute saline plus Tezosentan, a nonspecific endothelin antagonist. The drug was initially given as an intravenous bolus (10 mg/kg), followed by an infusion (2 mg/min) until the end of the experiment at 2 hours. Hemodynamic data were measured before APTE and then at 30-minute intervals. Pulmonary vascular resistance index (PVRI) was calculated as (Ppa-Pw)/CI, where CI was cardiac index or Qt/W (body weight). Fluorescent microspheres (FMS) were used to mark regional blood flows and ventilation for cluster analysis. PVRI acutely increased within minutes and remained high despite some recovery over time. With Tezosentan treatment, the results showed that endothelin-mediated vasoconstriction persisted significantly up to 2 hours and accounted for about 25% of the increase in PVRI while clot obstruction accounted for the remaining 75%. CI remained relatively constant throughout. Tezosentan also affected PVRI indirectly by mitigating the shift of regional blood flow back to the embolized areas over time, possibly by attenuating vasoconstriction in the nonembolized areas. We conclude that following APTE, although the increased PVRI is mostly due to mechanical embolic obstruction, secondary factors such as vasoconstriction and pattern of regional blood flow over time also play important roles.

Long-term survival after lung transplantation is limited by acute and chronic graft rejection. Induction of immune tolerance by first establishing mixed hematopoietic chimerism (MC) is a promising strategy to improve outcomes. In a preclinical canine model, stable MC was established in recipients after reduced-intensity conditioning and hematopoietic cell transplantation from a DLA-identical donor. Delayed lung transplantation was performed from the stem cell donor without pharmacological immunosuppression. Lung graft survival without loss of function was prolonged in chimeric (n = 5) vs. nonchimeric (n = 7) recipients (por = 0.05, Fisher's test). There were histological changes consistent with low-grade rejection in 3/5 of the lung grafts in chimeric recipients ator =1 year. Chimeric recipients after lung transplantation had a normal immune response to a T-dependent antigen. Compared to normal dogs, there were significant increases of CD4+INFgamma+, CD4+IL-4+ and CD8+ INFgamma+ T-cell subsets in the blood (p0.0001 for each of the three T-cell subsets). Markers for regulatory T-cell subsets including foxP3, IL10 and TGFbeta were also increased in CD3+ T cells from the blood and peripheral tissues of chimeric recipients after lung transplantation. Establishing MC is immunomodulatory and observed changes were consistent with activation of both the effector and regulatory immune response.

Studies in whole animals, isolated lungs and pulmonary tissue strips have shown that the pulmonary vascular resistance (PVR) to hypoxia is temporally biphasic in nature. We studied the regional temporal response to hypoxia in prone pigs. The animals were ventilated with an FIO2 of 0.21 (control), followed by an FIO2 of 0.12 for 180 min. A biphasic response in P(pa) to hypoxia was seen with the first peak between 10 and 20 min and a second rise in P(pa) starting after 30 min, which was due to an increase in cardiac output. Regional blood flow (Q ) and ventilation (V (A)) were measured using i.v. infusion of 15 microm and inhalation of 1 microm fluorescent microspheres, respectively. We grouped the lung pieces according to their temporal relative flow response to hypoxia. The five groups were each spatially distributed similarly, but not identically, among the animals. The corresponding relative ventilation to each group did not vary much. We conclude that in the prone pig, the PVR response to sustained hypoxia varies among regions of the lungs. Following an initial rise in PVR in most lung pieces, we found unexpectedly that some regions continue to increase PVR progressively and while other regions decrease PVR after the initial increase. The net effect is little change of overall PVR to hypoxia with time. Normoxic control animals had little change in their hemodynamics and the large majority of the lung pieces did not change their resistance over 3h. We speculate that the differential response of regions may be due to a differential role of nitric oxide, endothelin-1 release or K(+) channels.

Study objectives Hypercapnic acidosis has antiinflammatory effects in animal models of acute lung injury (ALI) and improves ventilation-perfusion (V/Q) matching in normal lungs. The effect of hypercapnia on V/Q matching in ALI is conflicting. Hypercapnic acidosis produced by reduced tidal volumes (V t s) was associated with an increased shunt fraction (QS/QT) in patients with ALI compared with control subjects. V t differences between groups make the assessment of hypercapnic acidosis on V/Q matching difficult. Adding CO 2 to the inhaled gas allows the comparison of gas exchange under identical V t conditions. We hypothesized the presence of hypercapnic acidosis from inspired carbon dioxide (ICD) would improve gas exchange in ALI and would be superior to that of low minute ventilation (LV e ) produced by reduced respiratory rate, rather than V t . Design University laboratory study of anesthetized New Zealand White rabbits. Interventions Assessment of V/Q relationships using the multiple inert gas elimination technique was performed in 10 saline solution-lavaged animals, which were ventilated with 6 mL/kg V t s and a positive end-expiratory pressure of 8 cm H 2 O. Each rabbit was studied while it was in eucapnia, followed by hypercapnia (Pa co 2 , 95 to 100 mm Hg) induced by LV e from decreased respiratory rate and by 10% ICD, in random order. Measurements and results The Pa o 2 was greater in ICD and LV e compared to eucapnia, but no significant differences in alveolar-arterial oxygen pressure difference or Pao 2 /fraction of inspired oxygen ratio occurred. LV e statistically reduced the mean V/Q distributions compared with ICD and eucapnia. Log SDs of ventilation and combined retention and excretion curves of the dispersion index were both increased during LV e , indicating the presence of unfavorable changes in ventilation distribution. Neither LV e nor ICD altered the QS/QT. Conclusions LV e slightly impairs overall gas exchange and ventilation distribution, but does not increase QS/QT compared with eucapnia and ICD. While ICD does not significantly improve gas exchange, it may be superior to LV e in achieving the antiinflammatory effects of “therapeutic” hypercapnia, since it does not adversely alter gas exchange and has the potential to make the lung more uniformly acidotic.

Exhaled acetone is measured to estimate exposure or monitor diabetes and congestive heart failure. Interpreting this measurement depends critically on where acetone exchanges in the lung. Health professionals assume exhaled acetone originates from alveolar gas exchange, but experimental data and theoretical predictions suggest that acetone comes predominantly from airway gas exchange. We measured endogenous acetone in the exhaled breath to evaluate acetone exchange in the lung. The acetone concentration in the exhalate of healthy human subjects was measured dynamically with a quadrupole mass spectrometer and was plotted against exhaled volume. Each subject performed a series of breathing maneuvers in which the steady exhaled flow rate was the only variable. Acetone phase III had a positive slope (0.054 ± 0.016 liter−1) that was statistically independent of flow rate. Exhaled acetone concentration was normalized by acetone concentration in the alveolar air, as estimated by isothermal rebreathing. Acetone concentration in the rebreathed breath ranged from 0.8 to 2.0 parts per million. Normalized end-exhaled acetone concentration was dependent on flow and was 0.79 ± 0.04 and 0.85 ± 0.04 for the slow and fast exhalation rates, respectively. A mathematical model of airway and alveolar gas exchange was used to evaluate acetone transport in the lung. By doubling the connective tissue (epithelium + mucosal tissue) thickness, this model predicted accurately ( R2 = 0.94 ± 0.05) the experimentally measured expirograms and demonstrated that most acetone exchange occurred in the airways of the lung. Therefore, assays using exhaled acetone measurements need to be reevaluated because they may underestimate blood levels.

Hypoxic pulmonary vasoconstriction (HPV) is known to affect regional pulmonary blood flow distribution. It is unknown whether lungs with well-matched ventilation (V̇)/perfusion (Q̇) have regional differences in the HPV response. Five prone pigs were anesthetized and mechanically ventilated (positive end-expiratory pressure = 2 cmH2O). Two hypoxic preconditions [inspired oxygen fraction (FiO2) = 0.13] were completed to stabilize the animal's hypoxic response. Regional pulmonary blood Q̇ and V̇ distribution was determined at various FiO2 (0.21, 0.15, 0.13, 0.11, 0.09) using the fluorescent microsphere technique. Q̇ and V̇ in the lungs were quantified within 2-cm3 lung pieces. Pieces were grouped, or clustered, based on the changes in blood flow when subjected to increasing hypoxia. Unique patterns of Q̇ response to hypoxia were seen within and across animals. The three main patterns (clusters) showed little initial difference in V̇/Q̇ matching at room air where the mean V̇/Q̇ range was 0.92–1.06. The clusters were spatially located in cranial, central, and caudal portions of the lung. With decreasing FiO2, blood flow shifted from the cranial to caudal regions. We determined that pulmonary blood flow changes, caused by HPV, produced distinct response patterns that were seen in similar regions across our prone porcine model.

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

Hypoxic pulmonary vasoconstriction (HPV) is thought to protect gas exchange by decreasing perfusion to hypoxic regions. However, with global hypoxia, non-uniformity in HPV may cause over-perfusion to some regions, leading to high-altitude pulmonary edema. To quantify the spatial distribution of HPV and regional P O 2 ( P R O 2 ) among small lung regions (∼2.0 cm3), five prone beagles (∼8.3 kg) were anesthetized and ventilated (PEEP ∼ 2 cm H2O) with an F I O 2 of 0.21, then 0.50, 0.18, 0.15, and 0.12 in random order. Regional blood perfusion (Q), ventilation (VA) and calculated P R O 2 were obtained using iv infusion of 15 μm and inhalation of 1 μm fluorescent microspheres. Lung pieces were clustered by their relative blood flow response to each F I O 2 . Clusters were shown to be spatially grouped within animals and across animals. Lung piece resistance increased as P R O 2 decreased to 60–70 mmHg but dropped at P R O 2 ’ s 60 mmHg. Regional ventilation changed little with hypoxia. HPV varied more in strength of response, rather than P R O 2 response threshold. In initially homogeneous VA/Q lungs, we conclude that HPV response is heterogeneous and spatially clustered.

Hypoxic pulmonary vasoconstriction (HPV) serves to maintain optimal gas exchange by decreasing perfusion to hypoxic regions. However, global hypoxia and nonuniform HPV may result in overperfusion of poorly constricted regions leading to local edema seen in high-altitude pulmonary edema. To quantify the spatial distribution of HPV and its response to regional Po2 (PrO2) among small lung regions, five pigs were anesthetized and mechanically ventilated in the supine posture. The animals were ventilated with an inspired O2 fraction (FiO2) of 0.50 and 0.21 and then (in random order) 0.15, 0.12, and 0.09. Regional blood flow (Q̇) and alveolar ventilation (V̇a) were measured by using intravenous infusion of 15 μm and inhalation of 1-μm fluorescent microspheres, respectively. PrO2 was calculated for each piece at each FiO2. Lung pieces differed in their Q̇ response to hypoxia in a manner related to their initial V̇a/Q̇ with FiO2 = 0.21. Reducing FiO2 < 0.15 decreased Q̇ to the initially high V̇a/Q̇ (higher PrO2) regions and forced Q̇ into the low V̇a/Q̇ (dorsal-caudal) regions. Resistance increased in most lung pieces as PrO2 decreased, reaching a maximum resistance when PrO2 is between 40 and 50 Torr. Local resistance decreased at Pro2 < 40 Torr. Pieces were statistically clustered with respect to their relative Q̇ response pattern to each FiO2. Some clusters were shown to be spatially organized. We conclude that HPV is spatially heterogeneous. The heterogeneity of Q̇ response may be related, in part, to the heterogeneity of baseline V̇a/Q̇.

Pulmonary arterial occlusion pressure is not thought to reflect left atrial pressure (Pla) when alveolar pressure (PA) exceeds pulmonary venous pressure because alveolar capillaries collapse and the required continuous fluid column between the pulmonary artery and left atrium is interrupted. However, arterial-to-venous flow can occur when PA exceeds both the pulmonary arterial pressure (Ppa) and pulmonary venous pressure (i.e., in Zone 1 conditions), indicating the existence of a continuous patent vascular channel. Accordingly, Ppa should reflect Pla under these conditions. To investigate this connection cannulas were placed in the pulmonary arteries and left atria of eight excised rabbit lungs. Ppa and Pla were set 5 cm H2O above PA, which ranged from 0 to 25 cm H2O. Pla was then reduced in 2 to 4 cm H2O decrements while recording Ppa when arterial-to-venous flow ceased. At all PAs greater than 0 cm H2O, Pla was accurately reflected by the Ppa when both were exceeded by PA. The greater the PA, the lower the Ppa could track Pla below PA. Pla can be accurately measured by a pulmonary arterial catheter under Zone 1 conditions.

We propose a model to measure both regional ventilation (V˙) and perfusion (Q˙) in which the regional radiodensity (RD) in the lung during xenon (Xe) washin is a function of regional V˙ (increasing RD) and Q˙(decreasing RD). We studied five anesthetized, paralyzed, mechanically ventilated, supine sheep. Four 2.5-mm-thick computed tomography (CT) images were simultaneously acquired immediately cephalad to the diaphragm at end inspiration for each breath during 3 min of Xe breathing. Observed changes in RD during Xe washin were used to determine regional V˙ and Q˙. For 16 mm3, Q˙ displayed more variance than V˙: the coefficient of variance of Q˙ (CVQ˙) = 1.58 ± 0.23, the CV of V˙ (CVV˙) = 0.46 ± 0.07, and the ratio of CVQ˙ to CVV˙ = 3.5 ± 1.1. CVQ˙(1.21 ± 0.37) and the ratio of CVQ˙ to CVV˙ (2.4 ± 1.2) were smaller at 1,000-mm3 scale, but CVV˙ (0.53 ± 0.09) was not. V˙/Q˙ distributions also displayed scale dependence: log SD of V˙ and log SD of Q˙ were 0.79 ± 0.05 and 0.85 ± 0.10 for 16-mm3 and 0.69 ± 0.20 and 0.67 ± 0.10 for 1,000-mm3 regions of lung, respectively. V˙ and Q˙ measurements made with CT and Xe also demonstrate vertically oriented and isogravitational heterogeneity, which are described using other methodologies. Sequential images acquired by CT during Xe breathing can be used to determine both regional V˙ and Q˙ noninvasively with high spatial resolution.

Hyperventilation with mixtures of O2 and CO2 has long been known to enhance carbon monoxide (CO) elimination at low HbCO levels in animals and humans. The effect of this therapy on oxygen delivery (DO2) has not been studied. Isocapnic hyperventilation utilizing mechanical ventilation may decrease cardiac output and therefore decrease DO2 while increasing CO elimination. We studied the effects of isocapnic hyperventilation on five adult mechanically ventilated sheep exposed to multiple episodes of severe CO poisoning. Five ventilatory patterns were studied: baseline minute ventilation (RR. VT), twice (2. RR) and four times (4. RR) baseline respiratory rate, and twice (2. VT) and four times (4. VT) baseline tidal volume. The mean carboxyhemoglobin (HbCO) washout half-time (t1/2) was 14.3 +/- 1.6 min for RR. VT, decreasing to 9.5 +/- 0.9 min for 2. RR, 8.0 +/- 0.5 min for 2. VT, 6.2 +/- 0.5 min for 4. RR, and 5.2 +/- 0.5 min for 4. VT. DO2 was increased during hyperventilation compared with baseline ventilation for 2. VT, 4. RR, and 4. VT ventilatory patterns. Isocapnic hyperventilation, in our animal model, did not alter arterial or pulmonary blood pressures, arterial pH, or cardiac output. Isocapnic hyperventilation is a promising therapy for CO poisoning.

The microsphere method has been used extensively to measure regional blood flow in large laboratory animals. A fundamental premise of the method is that microspheres do not alter regional flow or vascular tone. Whereas this assumption is accepted in large animals, it may not be valid in the pulmonary circulation of smaller animals. Three studies were performed to determine the hemodynamic effects of microspheres on the rat pulmonary circulation. Increasing numbers of 15-μm-diameter microspheres were injected into a fully dilated, isolated-lung preparation. Vascular resistance increased 0.8% for every 100,000 microspheres injected. Microspheres were also injected into an isolated-lung preparation in which vascular tone was increased with hypoxia. Microspheres did not induce vasodilatation, as reported in other vascular beds. Fluorescent microspheres were injected via tail veins into awake rats, and the spatial locations of the microspheres were determined. Regional distributions remained highly correlated when microspheres of one color were injected after microspheres of another color. This indicates that the initial injection did not alter regional perfusion. We conclude that, when used in appropriate numbers, 15-μm-diameter microspheres do not alter regional flow or vascular tone in the rat pulmonary circulation.

We used various ovalbumin sensitization and challenge protocols to determine the importance of the route of allergen administration and the genetic background in modulating the physiologic, inflammatory, and immunologic features characteristic of allergen-induced asthma. In BALB/c mice, induction of maximal airway hyperresponsiveness and airspace eosinophilia required administration of ovalbumin by both the intraperitoneal and the intranasal routes (combination protocol), whereas intraperitoneal immunization alone resulted in maximal ovalbumin-specific IgE plasma levels. Thus, a systemic immune response to allergen, in addition to, or independent of IgE production, as well as local allergen challenge were necessary for maximal induction of pulmonary disease. BALB/c mice treated with ovalbumin by the combination protocol had increased Th2-type cytokine mRNA levels in bronchial lymph node tissue compared with control mice. In contrast, C57BL/6 mice treated with ovalbumin by the combination protocol had significantly decreased responses compared with BALB/c mice for all parameters of allergic pulmonary disease examined, with the exception of airspace eosinophilia. Genetic background has a striking and selective effect on the phenotype of murine allergic pulmonary disease. Further analysis of this murine model should be useful in helping define the critical pathogenetic events in allergen-induced asthma.

Total liquid ventilation (LV) lowers airway pressures and potentially reduces barotrauma in models of hyaline membrane disease. LV eliminates surface tension by eliminating the air-perfluorochemicals (PFC) interface but does not eliminate interfacial tension (IT) at the lung/PFC interface. We hypothesized that pretreatment with exogenous surfactant before LV would shift the overall pressure-volume (PV) curve to the left, compared with LV without surfactant. Sequential quasi-static PV curves were obtained in 10 excised lungs (saline, air, PFC), with one-half randomized to exogenous surfactant replacement before LV. Analysis revealed that maximal inflation pressures were reduced during LV compared with baseline air curves. Addition of exogenous surfactant to LV further reduced maximal inflation pressures. A novel approach was used to transform these PV curves to estimates of in situ IT-volume curves. Estimated maximal IT at 20 ml/kg in preterm lamb lungs on air inflation after surfactant was 51 mN/m, compared with 40 mN/m for LV alone and with 27 mN/m for the combination of surfactant and LV. We conclude that the IT-reducing properties of the PFC studied (perflubron) can be augmented through the use of exogenous surfactant.

Airway hyperreactivity is defined as an increased bronchoconstrictor response to physical, pharmacological, or other stimuli. Patients with asthma develop airway hyperreactivity as well as peribronchial inflammation. We employed an established schistosome soluble egg antigen (SEA)-induced murine model of allergic inflammation to examine the temporal relationship between airway hyperreactivity and leukocyte subset infiltration. Dose response curves of intravenous methacholine were used in mice to characterize airway reactivity at various time points after intranasal SEA rechallenge. Cellular infiltration into the airspace was assessed by bronchoalveolar lavage. Airway hyperreactivity increased as early as 1 h postchallenge. Peak hyperreactivity occurred at 8 h postchallenge. Subsequently, reactivity decreased at 24 h and fell to the level observed in controls by 48 h. Neutrophil influx correlated directly with the increase in airway reactivity, as neutrophils were observed as early as 1 h, peaked at 8 h, diminished by 24 h and were not detected at 48 h post-SEA challenge. In contrast, eosinophil infiltration was not observed until 24 h and peaked at 48 h post-SEA rechallenge when increases in airway reactivity were not detected. Airway resistance induced by methacholine correlated with neutrophil (r2 = 0.90) but not eosinophil (r2 = 0.1) infiltration. These results suggest that the airway hyperreactivity observed during allergic airway inflammation correlates with airways neutrophilia and weakly eosinophil accumulation.

In the current study, we used a canine model of radiation-induced lung injury to test the effect of a single i.v. infusion of 10×10(6)/kg of marrow fibroblasts on the progression of damage following 15 Gy exposure to the right lung. The fibroblasts, designated DS1 cells, are a cloned population of immortalized cells isolated from a primary culture of marrow stromal cells. DS1 cells were infused at week 5 post-irradiation when lung damage was evident by imaging with high-resolution computed tomography (CT). At 13 weeks post-irradiation we found that 4 out of 5 dogs receiving DS1 cells had significantly improved pulmonary function compared to 0 out of 5 control dogs (p = 0.047, Fisher's Exact). Pulmonary function was measured as the single breath diffusion capacity-hematocrit (DLCO-Hct), the total inspiratory capacity (IC), and the total lung capacity (TLC), which differed significantly between control and DS1-treated dogs; p = 0.002, p = 0.005, and p = 0.004, respectively. The DS1-treated dogs also had less pneumonitis detected by CT imaging and an increased number of TTF-1 (thyroid transcription factor 1, NKX2-1) positive cells in the bronchioli and alveoli compared to control dogs. Endothelial-like progenitor cells (ELC) of host origin, detected by colony assays, were found in peripheral blood after DS1 cell infusion. ELC numbers peaked one day after infusion, and were not detectable by 7 days. These data suggest that infusion of marrow fibroblasts stimulates mobilization of ELC, which is associated with a reduction in otherwise progressive radiation-induced lung injury. We hypothesize that these two observations are related, specifically that circulating ELC contribute to increased angiogenesis, which facilitates endogenous lung repair.

We compared the effects of pulsatile vs. nonpulsatile flow (Q) on pulmonary arterial pressure (Ppa)-Q relationships in zone 3 over wide ranges of pulse rate, stroke volume (SV), and Q. Excised left lungs of rabbits (n = 15) were perfused with tris(hydroxymethyl)aminomethane-buffered Tyrode solution containing 4% dextran, 1% albumin, and 10 mg/l of indomethacin and were ventilated with room air. Pulsatile Q was generated by a diaphragm pump delivering SV of 0.5, 1, or 2 ml (representing approximately 0.3, 0.6, and 1.2 times, respectively, the normal resting SV for rabbit left lung) and adjusting the pump frequency. Nonpulsatile Q was generated by raising an arterial reservoir to the required height. Mean pulmonary arterial (Ppa) and left atrial pressures were measured at end exhalation (positive end-expiratory pressure = 2.5 cmH2O) near the tips of the perfusion cannulas and were referenced to the lung base. Left atrial pressure was held constant at 7 cmH2O.Q was alternated between pulsatile and nonpulsatile, increasing Q stepwise from 100 to 600 ml/min (Q from approximately 0.3 to 2 times the normal resting Q for rabbit left lung), after which Q was reduced stepwise back to initial values. For the smallest SV there were no differences between Ppa-Q curves under pulsatile and nonpulsatile conditions. At the largest SV, Ppa was greater during pulsatile than nonpulsatile Q at Q > 100 ml/min. The slopes of the Ppa-Q curves were greater during pulsatile Q at the two larger SV values. These results can be explained by increasing Q turbulence and less ideal velocity profiles at higher peak Q resulting from the effects of rapidly changing inertial forces.

Real-time imaging of cellular and sub-cellular dynamics in vascularized organs requires image-resolution, image-registration, and demonstrably intact physiology to be simultaneously optimized. This problem is particularly pronounced in the lung in which cells may transit at speeds > 1 mm/sec, and in which normal respiration results in large-scale tissue movements that prevent image registration. Here, we report video-rate, two-photon imaging of a physiologically intact preparation of the mouse lung that is at once stabilizing and non-disruptive. The application of our method provides evidence for differential trapping of T cells and neutrophils in mouse pulmonary capillaries and enables observation of neutrophil mobilization and dynamic vascular leak in response to stretch and inflammatory models of lung injury in mice. The system permits physiological measurement of motility rates of > 1 mm/sec, observation of detailed cellular morphology, and could be applied to other organs and tissues while maintaining intact physiology.

We utilized microfocal fluoroscopic angiography to study the influence of lung inflation on small (0.2- to 1.3-mm-diam) pulmonary arteries in isolated left lower lobes from dog lungs during both flow and no-flow conditions. Alveolar pressure, which in this preparation was equal to transpulmonary pressure, was set at 2, 8, or 14 mmHg while vascular pressure was varied from 0 to 24 mmHg. The diameters of these small arterial vessels increased with lung inflation. No differences were observed between the results obtained during flow and no-flow conditions. Thus, arteries in this diameter range can be considered as extra-alveolar, and the effect of lung inflation on these small extra-alveolar arteries was qualitatively similar to that previously described for larger extra-alveolar vessels. Quantitatively, the degree of vessel distension was about the same per unit increase in transpulmonary pressure at constant vascular pressure as for a change in vascular pressure at constant transpulmonary pressure. Accordingly, inflation produced a decrease in perivascular pressure surrounding these small arteries that was approximately equal to the increase in transpulmonary pressure.

The effect of severe generalized edema on respiratory system mechanics is not well described. We measured airway pressure, gastric pressure, and four vertical pleural pressures in 13 anesthetized paralyzed pigs ventilated in the upright position. Pressure-volume relationships of the respiratory system, chest wall, and lung were measured on deflation from total lung capacity to residual volume and during tidal breathing both before (control) and 50 min after one of two interventions. In one series of experiments, a volume equal to 15–20% of the pig's body weight was infused intravenously. In a second series, a balloon was placed in the peritoneal space to distend the abdomen to the same gastric pressures as achieved in the first series. Measurements were compared before and after either abdominal balloon inflation or volume infusion. Volume infusion increased the pleural pressure in dependent lung regions, decreased both total lung capacity (34%) and functional residual capacity (62%) (both P less than 0.05), and markedly shifted the respiratory system and chest wall pressure-volume curves to the right, but it only moderately affected the lung deflation curve. Tidal compliances of the respiratory system, chest wall, and lung decreased 36, 31, and 49%, respectively (all P less than 0.05). The effect of abdominal balloon inflation on respiratory system mechanics was similar to that of volume infusion. We conclude that infusing large volumes of fluid markedly alters chest wall mechanics, mainly by causing abdominal distension that prohibits descent of the diaphragm.

Previous studies reported that regional CO2tension might affect regional ventilation (V̇) following acute pulmonary thromboembolism (APTE). We investigated the pathophysiology and magnitude of these changes. Eight anesthetized and ventilated piglets received autologous clots at time = 0 min until mean pulmonary artery pressure was 2.5 times baseline. The distribution of V̇ and perfusion (Q̇) at four different times (−5, 30, 60, 120 min) was mapped by fluorescent microspheres. Regional V̇ and Q̇ were examined postmortem by sectioning the air-dried lung into 900–1,000 samples of ∼2 cm3each. After the redistribution of regional Q̇ by APTE, but in the scenario assuming that no V̇ shift had yet occurred, CO2tension in different lung regions at 30 min post-APTE (PXCO2) was estimated from the V̇/Q̇ data and divided into four distinct clusters: i.e., PXCO2< 10 Torr; 10 < PXCO2< 25 Torr; 25 < PXCO2< 50 Torr; PXCO2> 50 Torr. Our data showed that the clusters in higher V̇/Q̇ regions (with a PXCO2< 25 Torr) received ∼35% less V̇ when measured within 30 min of APTE, whereas, in contrast, the lower V̇/Q̇ regions showed no statistically significant increases in their V̇. However, after 30 min, there was minimal further redistribution of V̇. We conclude that there are significant compensatory V̇ shifts out of regions of low CO2tension soon following APTE, and that these variations in regional CO2tension, which initiate CO2-dependent changes in airway resistance and lung parenchymal compliance, can lead to improved gas exchange.

Regional pulmonary blood flow in dogs under zone 3 conditions was measured in supine and prone postures to evaluate the linear gravitational model of perfusion distribution. Flow to regions of lung that were 1.9 cm3 in volume was determined by injection of radiolabeled microspheres in both postures. There was marked perfusion heterogeneity within isogravitational planes (coefficient of variation = 42.5%) as well as within gravitational planes (coefficient of variation = 44.2 and 39.2% in supine and prone postures, respectively; P = 0.02). On average, vertical height explained only 5.8 and 2.4% of the flow variability in the supine and prone postures, respectively. Whereas the gravitational model predicts that regional flows should be negatively correlated when measured in supine and prone postures, flows in the two postures were positively correlated, with an r2 of 0.708 +/- 0.050. Regional perfusion as a function of distance from the center of a lung explained 13.4 and 10.8% of the flow variability in the supine and prone postures, respectively. A linear combination of vertical height and radial distance from the centers of each lung provided a better-fitting model but still explained only 20.0 and 12.0% of the flow variability in the supine and prone postures, respectively. The entire lung was searched for a region of contiguous lung pieces (22.8 cm3) with high flow. Such a region was found in the dorsal area of the lower lobes in six of seven animals, and flow to this region was independent of posture. Under zone 3 conditions, neither gravity nor radial location is the principal determinant of regional perfusion distribution in supine and prone dogs.

Abdominal distension (AD) occurs in pregnancy and is also commonly seen in patients with ascites from various causes. Because the abdomen forms part of the "chest wall," the purpose of this study was to clarify the effects of AD on ventilatory mechanics. Airway pressure, four (vertical) regional pleural pressures, and abdominal pressure were measured in five anesthetized, paralyzed, and ventilated upright pigs. The effects of AD on the lung and chest wall were studied by inflating a liquid-filled balloon placed in the abdominal cavity. Respiratory system, chest wall, and lung pressure-volume (PV) relationships were measured on deflation from total lung capacity to residual volume, as well as in the tidal breathing range, before and 15 min after abdominal pressure was raised. Increasing abdominal pressure from 3 to 15 cmH2O decreased total lung capacity and functional residual capacity by approximately 40% and shifted the respiratory system and chest wall PV curves downward and to the right. Much smaller downward shifts in lung deflation curves were seen, with no change in the transdiaphragmatic PV relationship. All regional pleural pressures increased (became less negative) and, in the dependent region, approached 0 cmH2O at functional residual capacity. Tidal compliances of the respiratory system, chest wall, and lung were decreased 43, 42, and 48%, respectively. AD markedly alters respiratory system mechanics primarily by "stiffening" the diaphragm/abdomen part of the chest wall and secondarily by restricting lung expansion, thus shifting the lung PV curve as seen after chest strapping. The less negative pleural pressures in the dependent lung regions suggest that nonuniformities of ventilation could also be accentuated and gas exchange impaired by AD.

We have previously observed flows equivalent to 15% of the resting cardiac output of rabbits occurring through isolated lungs that were completely in zone 1. To distinguish between alveolar corner vessels and alveolar septal vessels as a possible zone 1 pathway, we made in vivo microscopic observations of the subpleural alveolar capillaries in five anesthetized dogs. Videomicroscopic recordings were made via a transparent thoracic window with the animal in the right lateral position. From recordings of the uppermost surface of the left lung, alveolar septal and corner vessels were classified depending on whether they were located within or between alveoli, respectively. Observations were made with various levels of positive end-expiratory pressure (PEEP) applied only to the left lung via a double-lumen endotracheal tube. Consistent with convention, flow through septal vessels stopped when PEEP was raised to the mean pulmonary arterial pressure (the zone 1-zone 2 border). However, flow through alveolar corner vessels continued until PEEP was 8-16 cmH2O greater than mean pulmonary arterial pressure (8-16 cm into zone 1). These direct observations support the idea that alveolar corner vessels rather than patent septal vessels provide the pathway for blood flow under zone 1 conditions.

We performed a multicenter study to test the hypothesis that tidal liquid ventilation (TLV) would improve cardiopulmonary, lung histomorphological, and inflammatory profiles compared with conventional mechanical gas ventilation (CMV). Sheep were studied using the same volume-controlled, pressure-limited ventilator systems, protocols, and treatment strategies in three independent laboratories. Following baseline measurements, oleic acid lung injury was induced and animals were randomized to 4 hours of CMV or TLV targeted to "best PaO2" and PaCO2 35 to 60 mm Hg. The following were significantly higher (p < 0.01) during TLV than CMV: PaO2, venous oxygen saturation, respiratory compliance, cardiac output, stroke volume, oxygen delivery, ventilatory efficiency index; alveolar area, lung % gas exchange space, and expansion index. The following were lower (p < 0.01) during TLV compared with CMV: inspiratory and expiratory pause pressures, mean airway pressure, minute ventilation, physiologic shunt, plasma lactate, lung interleukin-6, interleukin-8, myeloperoxidase, and composite total injury score. No significant laboratories by treatment group interactions were found. In summary, TLV resulted in improved cardiopulmonary physiology at lower ventilatory requirements with more favorable histological and inflammatory profiles than CMV. As such, TLV offers a feasible ventilatory alternative as a lung protective strategy in this model of acute lung injury.

SUMMARY We tested the hypothesis that surfactant replacement would be beneficial In the acld­ aspiration model of acute lung Injury. HCI (0.1 N, 2 mllkg) was Injected Into the trachea of excised rabbit lungs (n = 8). Control lungs (n = 4) had no Intervention. All were perfused with lYrode's solution mixed 1:1 with autologous whole blood at 40 mllmin/kg for 30 min, and then degassed. A modified natural surfactant (Survanta@, Ross Laboratories) was then Injected Into the trachea of four lungs Injured with HCI (100 mg/kg at 25 mg/ml). lWo quasi-static pressure-volume curves were determined. The mean alveolar pressures at 50,60,70,80, and 90% of TLC were greater In the HCI group than In the control group (p < 0.05). However, no difference was observed between the control lungs and thosethat received HCI + Survanta. In 13 anesthetized, paralyzed, and venti­ lated rabbits, deflation pressure-volume curvas were determined from TLC to FRC (measured by helium dilution). Then, 0.1 N HCI (3 ml/kg) was Injected into the trachea and, in seven, Survanta was Instilled 5 min later. The mean alveolar pressures at 60, 70, 80, and 90% TLC were higher at 15 and 60 min In the HCI group compared with their pre-HCI time point (p < 0.05). In the HCI + Survanta group, no differences were seen at 15 min, and only slight Increased were seen at 60 min. No effect of surfactant replacement on arterial blood gases was observed. HCI aspiration Increased recoil In both excised and in "i"o lungs, and surfactant replacement with Survanta returned recoil to normal. AM REV RESPIR DIS 1990; 142:1279-1283

We studied the roles of endothelins in determining ventilation (V̇a) and perfusion (Q̇) mismatch in a porcine model of acute pulmonary thromboembolism (APTE), using a nonspecific endothelin antagonist, tezosentan. Nine anesthetized piglets (∼23 kg) received autologous clots (∼20 g) via a central venous catheter at time = 0 min. The distribution of V̇a and Q̇ at five different time points (−30, −5, 30, 60, 120 min) was mapped by fluorescent microspheres of 10 different colors. Five piglets ( group 1) received tezosentan (courtesy of Actelion) starting at time = 40 min for 2 h, and four piglets ( group 2) received only saline and served as control. Our results showed that, in all of the animals at 30 min following APTE but before tezosentan, the mean V̇a/Q̇ was increased, as was V̇a/Q̇ heterogeneity (log SD V̇a/Q̇), which represented a widening of its main peak. Afterwards, tezosentan attenuated the pulmonary hypertension in group 1 but also produced moderate systemic hypotension. However, it did not improve arterial Po2 or V̇a/Q̇ mismatch. We concluded that endothelin antagonism had minimal impact on gas exchange following APTE and confirmed our earlier observation that the main mechanism for hypoxemia in APTE was due to the mechanical redistribution of pulmonary regional blood flow away from the embolized vessels, resulting in the creation of many divergent low and high V̇a/Q̇ regions.

Hypercapnic acidosis has antiinflammatory effects in animal models of acute lung injury (ALI) and improves ventilation-perfusion (V/Q) matching in normal lungs. The effect of hypercapnia on V/Q matching in ALI is conflicting. Hypercapnic acidosis produced by reduced tidal volumes (Vts) was associated with an increased shunt fraction (QS/QT) in patients with ALI compared with control subjects. Vt differences between groups make the assessment of hypercapnic acidosis on V/Q matching difficult. Adding CO2 to the inhaled gas allows the comparison of gas exchange under identical Vt conditions. We hypothesized the presence of hypercapnic acidosis from inspired carbon dioxide (ICD) would improve gas exchange in ALI and would be superior to that of low minute ventilation (LVe) produced by reduced respiratory rate, rather than Vt.University laboratory study of anesthetized New Zealand White rabbits.Assessment of V/Q relationships using the multiple inert gas elimination technique was performed in 10 saline solution-lavaged animals, which were ventilated with 6 mL/kg Vts and a positive end-expiratory pressure of 8 cm H2O. Each rabbit was studied while it was in eucapnia, followed by hypercapnia (Pa(CO2), 95 to 100 mm Hg) induced by LVe from decreased respiratory rate and by 10% ICD, in random order.The Pa(O2) was greater in ICD and LVe compared to eucapnia, but no significant differences in alveolar-arterial oxygen pressure difference or Pa(O2)/fraction of inspired oxygen ratio occurred. LVe statistically reduced the mean V/Q distributions compared with ICD and eucapnia. Log SDs of ventilation and combined retention and excretion curves of the dispersion index were both increased during LVe, indicating the presence of unfavorable changes in ventilation distribution. Neither LVe nor ICD altered the QS/QT.LVe slightly impairs overall gas exchange and ventilation distribution, but does not increase QS/QT compared with eucapnia and ICD. While ICD does not significantly improve gas exchange, it may be superior to LVe in achieving the antiinflammatory effects of "therapeutic" hypercapnia, since it does not adversely alter gas exchange and has the potential to make the lung more uniformly acidotic.

We have shown previously that inspired CO2 (3-5%) improves ventilation-perfusion (V̇a/Q̇) matching but with the consequence of mild arterial hypercapnia and respiratory acidosis. We hypothesized that adding CO2 only late in inspiration to limit its effects to the conducting airways would enhance V̇a/Q̇ matching and improve oxygenation without arterial hypercapnia. CO2 was added in the latter half of inspiration in a volume aimed to reach a concentration of 5% in the conducting airways throughout the respiratory cycle. Ten mixed-breed dogs were anesthetized and, in a randomized order, ventilated with room air, 5% CO2 throughout inspiration, and CO2 added only to the latter half of inspiration. The multiple inert-gas elimination technique was used to assess V̇a/Q̇ heterogeneity. Late-inspired CO2 produced only very small changes in arterial pH (7.38 vs. 7.40) and arterial CO2 (40.6 vs. 39.4 Torr). Compared with baseline, late-inspired CO2 significantly improved arterial oxygenation (97.5 vs. 94.2 Torr), decreased the alveolar-arterial Po2 difference (10.4 vs. 15.7 Torr) and decreased the multiple inert-gas elimination technique-derived arterial-alveolar inert gas area difference, a global measurement of V̇a/Q̇ heterogeneity (0.36 vs. 0.22). These changes were equal to those with 5% CO2 throughout inspiration (arterial Po2, 102.5 Torr; alveolar-arterial Po2 difference, 10.1 Torr; and arterial-alveolar inert gas area difference, 0.21). In conclusion, we have established that the majority of the improvement in gas exchange efficiency with inspired CO2 can be achieved by limiting its application to the conducting airways and does not require systemic acidosis.

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

To compare the relative contributions of gravity and vascular structure to the distribution of pulmonary blood flow, we flew with pigs on the National Aeronautics and Space Administration KC-135 aircraft. A series of parabolas created alternating weightlessness and 1.8-G conditions. Fluorescent microspheres of varying colors were injected into the pulmonary circulation to mark regional blood flow during different postural and gravitational conditions. The lungs were subsequently removed, air dried, and sectioned into ∼2 cm3 pieces. Flow to each piece was determined for the different conditions. Perfusion heterogeneity did not change significantly during weightlessness compared with normal and increased gravitational forces. Regional blood flow to each lung piece changed little despite alterations in posture and gravitational forces. With the use of multiple stepwise linear regression, the contributions of gravity and vascular structure to regional perfusion were separated. We conclude that both gravity and the geometry of the pulmonary vascular tree influence regional pulmonary blood flow. However, the structure of the vascular tree is the primary determinant of regional perfusion in these animals.

Observations made on vessels seen directly beneath the pleura may not accurately reflect what occurs in vessels located deeper in the interior of the lung. We quantified flow to subpleural and deeper, interior regions under zone 1 or 2 conditions in excised ( n = 5) and in vivo ( n = 6) rabbit lungs, in the head-up or inverted position. After infusion of radiolabeled microspheres, lungs were dried at alveolar pressure of 25 cmH2O and sliced in 1-cm sections along the gravitational plane and in three planes in the dorsal-ventral axis. Regions located

Immunized mice after inhalation of specific antigen have the following characteristic features of human asthma: airway eosinophilia, mucus and Th2 cytokine release, and hyperresponsiveness to methacholine. A model of late-phase allergic pulmonary inflammation in ovalbumin-sensitized mice was used to address the role of the alpha4 integrin (CD49d) in mediating the airway inflammation and hyperresponsiveness. Local, intrapulmonary blockade of CD49d by intranasal administration of CD49d mAb inhibited all signs of lung inflammation, IL-4 and IL-5 release, and hyperresponsiveness to methacholine. In contrast, CD49d blockade on circulating leukocytes by intraperitoneal CD49d mAb treatment only prevented the airway eosinophilia. In this asthma model, a CD49d-positive intrapulmonary leukocyte distinct from the eosinophil is the key effector cell of allergen-induced pulmonary inflammation and hyperresponsiveness.

We previously found that up to 15% of the normal cardiac output can flow through lungs that are entirely in zone 1 and that the zone 1 pathway utilizes alveolar corner vessels. Because of the proximity of these vessels to alveoli, we hypothesized that lungs perfused under zone 1 conditions would exchange gas. We used the multiple inert gas elimination technique to assess the ventilation-perfusion (VA/Q) distribution under zones 1 and 2 in six rabbit lungs perfused with tris(hydroxymethyl)aminomethane-buffered Tyrode solution containing 1% albumin, 4% dextran, and papaverine (25 mg/l). High-frequency oscillation (tidal volume = 2.8 ml at 20 Hz, bias flow = 1 l/min) kept alveolar pressure (PA) nearly constant at 10 or 20 cmH2O. Pulmonary arterial pressure was set 2.5 cmH2O below or 5 cmH2O above PA (zones 1 and 2, respectively). Pulmonary venous pressure was kept at 0 cmH2O, with zero reference being the bottom of the lung. At PA of 10 cmH2O, flow was 64 +/- 40 and 5 +/- 3 ml/min (P < 0.05) and the mean VA/Q for perfusion was 1.1 +/- 0.4 and > 5 (P < 0.05) in zones 2 and 1, respectively. At PA of 20 cmH2O, flow was 89 +/- 36 and 22 +/- 13 ml/min (P < 0.05) and the mean VA/Q for perfusion was 0.8 +/- 0.3 and 3.7 +/- 2.4 (P < 0.05) in zones 2 and 1, respectively. Shunt averaged < 5% of total flow in all conditions. Blood flowing through vessels remaining open under zone 1 conditions 1) exchanges gas, 2) does not occur through anatomic or physiological shunts, and 3) may explain the high VA/Q seen with positive end-expiratory pressure.

We previously reported that mean pulmonary arterial pressure (Ppa) during pulsatile flow exceeded that for steady flow when flow was greater than the normal resting value and speculated that this was due to irregularities of the flow profiles in precapillary vessels, mainly the larger arteries. From this we hypothesized that neither mean microvascular pressure nor the rate of fluid filtration would be affected by flow pulsatility. We therefore compared the effects of steady vs. pulsatile flow on the double-occlusion pressure (Pdo) and on edema formation (rate of weight gain) in zone 3 rabbit lungs. Excised left lungs (n = 19) were perfused with Tyrode solution and ventilated with an end-expiratory pressure of 2.5 cmH2O. A diaphragm pump generated pulsatile flow with a stroke volume of 1.0 ml (approximately 0.8 the normal resting value for rabbit left lung). Nonpulsatile flow was generated by raising an arterial reservoir. Flow rate was set at 100 or 400 ml/min (approximately 0.4 or 1.6 x the normal resting cardiac output, respectively). Vascular pressures (referenced to the bottom of the lung) were measured after ventilation, at end expiration, was interrupted. Pdo values were obtained in random order at 15 time points that were evenly distributed within the pulse cycle, averaged across pulses to obtain the mean capillary pressure profile, and then averaged over time. At the lower flow of 100 ml/min, mean Ppa and Pdo were slightly lower (3–4%) during pulsatile compared with nonpulsatile conditions. At the higher flow of 400 ml/min, mean Ppa was higher under pulsatile conditions (13%), whereas downstream the mean Pdo values were equal.(ABSTRACT TRUNCATED AT 250 WORDS)

The mechanism by which oxygenation improves when patients with ARDS are turned from supine to prone position is not known. From results of our previous studies we reasoned that (1) when supine, in the setting of lung injury, transpulmonary pressure will be less than airway opening pressure and (2) atelectasis will develop preferentially in dorsal lung areas, and (3) both ventilation and ventilation/perfusion ratios would improve in these regions on turning prone. To study this directly, we measured regional ventilation and perfusion using 81mKr and 99mTc-MAA, respectively, and single photon emission computed tomography, both prone and supine, in four control animals and four given oleic acid. After oleic acid, the prone position improved (1) oxygenation (mean +/- SD PaO2 = 140 +/- 112 versus 453 +/- 54 mm Hg), (2) median ventilation/perfusion ratios (0.77 versus 0.95), (3) ventilation/perfusion heterogeneity (coefficient of variation 86 +/- 15 versus 61 +/- 6), and (4) the gravitational ventilation/perfusion gradient (dependent to non-dependent slopes of 0.22 versus -0.02, all p0.05). The prone position generates a transpulmonary pressure sufficient to exceed airway opening pressure in dorsal lung regions, i.e., in regions where atelectasis, shunt, and ventilation/perfusion heterogeneity are most severe, without adversely affecting ventral lung regions.

Oxygenation improves in patients with adult respiratory distress syndrome and in animals with oleic acid-induced lung injury when they are turned from the supine to the prone position. Dependent and nondependent pleural pressures (Ppl) were measured in six pigs ventilated in the supine and prone positions before and after volume infusion (VI). Before VI the mean +/- SEM AaPO2 difference was 26 +/- 8 mm Hg when the animals were supine and 10 +/- 2 mm Hg when they were prone (p > 0.05). After VI the AaPO2 was 64 +/- 6 mm Hg when the animals were supine (p < 0.05) and 43 +/- 7 mm Hg when they were prone (p < 0.05). VI increased the Ppl gradient from 0.53 +/- 0.1 to 0.71 +/- 0.1 cm H2O/cm when the animals were supine (p < 0.05) and from 0.17 +/- 0.1 to 0.27 +/- 0.1 cm H2O/cm when they were prone (p < 0.05). Dependent Ppl at FRC was much less positive when the animals were prone versus supine (0.9 +/- 0.3 versus 3.0 +/- 0.5 cm H2O, p < 0.05), suggesting that the airways in these dependent regions would narrow and/or close and that ventilation to these regions would diminish as a result of VI.

Unilateral pulmonary artery obstruction (PAO) for 24–48 h, followed by reperfusion, results in pulmonary edema and lung inflammation. We hypothesized that lung injury actually occurred during the period of PAO but, because of low microvascular pressures during the period of occlusion, was not detected until perfusion was reestablished. To test this hypothesis, we studied 14 rabbits divided into three groups: group I rabbits underwent sham occlusion of the left pulmonary artery for 24 h; group II rabbits underwent PAO but were not reperfused; and group III rabbits were subjected to PAO and then reperfused for 4 h. The fluid filtration coefficient measured during a zone 3 no-flow hydrostatic stress (pulmonary arterial pressure = pulmonary venous pressure, both greater than alveolar pressure) in group I lungs was less than that of lungs in either group II or III [0.52 +/- 0.02 (SE) ml.min-1.cmH2O.100 g wet wt-1 vs. 0.94 +/- 0.11 and 0.86 +/- 0.13 for groups II and III, respectively, P less than 0.05]. The wet-to-dry weight ratio of the left lung measured after the zone 3 stress was applied for 20 min was 6.90 +/- 0.09 in group I rabbits and 9.21 +/- 0.75 and 11.75 +/- 0.44 in groups II and III, respectively (P less than 0.05). Radiolabeled microspheres demonstrated that flow to the left lung was diminished after the period of PAO (38 +/- 4, 9 +/- 5, and 2 +/- 1% of cardiac output in groups I, II, and III, respectively; P less than 0.05 for group I vs. groups II and III).(ABSTRACT TRUNCATED AT 250 WORDS)

Fluid leaking from arterial and venous extra-alveolar vessels (EAV's) may account for up to 60% of the total transvascular fluid flux when edema occurs in the setting of normal vascular permeability. We determined if the permeability and relative contribution of EAV's was altered after inducing acute lung injury in rabbits by administering oleic acid (0.1 ml/kg) into the pulmonary artery, HCl (5 ml/kg of 0.1 N) into the trachea, or air emboli (0.03 ml.kg-1.min-1) into the right atrium for 90 min. Subsequently, the lungs were excised and continuously weighed while they were maintained in a warmed, humidified chamber with alveolar and pulmonary vascular pressures controlled and the lungs either ventilated or distended with 5% CO2 in air. The vascular system was filled with autologous blood and saline (1:1) to which papaverine (0.1 mg/ml) was added to inhibit vasospasm. Vascular pressures were referenced to the lung base. After a transient hydrostatic stress to maximize recruitment, vascular pressures were set at 5 cmH2O, and lungs were allowed to become isogravimetric (30-60 min). A fluid filtration coefficient (Kf) was determined by the use of a modification of the method of Drake and colleagues [Am. J. Physiol. 234 (Heart Circ. Physiol. 3): H266-H274, 1978]. EAV's were isolated by zoning techniques. In control preparations arterial and venous EAV's accounted for 26% (n = 9) and 38% (n = 11) of the total leakage, respectively. In all three models Kf increased two- to fourfold when the lungs were in zone 3 (alveolar vessels and arterial and venous EAV's contributing to the leakage).(ABSTRACT TRUNCATED AT 250 WORDS)

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)

Because of conflicting data in the literature, we studied the effect of positive-pressure inflation on transvascular fluid filtration in zone 1 lungs. Lungs from New Zealand White rabbits (n = 10) were excised, perfused with saline and autologous whole blood (1:1), ventilated, and continuously weighed. Pulmonary arterial and venous pressures (Pvas) were referenced to the most dependent part of the lung. A change in vascular volume (delta Vvas) and a fluid filtration rate (FFR) were calculated from the change in lung weight that occurred from 0 to 30 s and from 3 to 5 and 5 to 10 min, respectively, after changing alveolar pressure (PA). FFR's and delta Vvas's were measured with Pvas equal to 2 or 10 cmH2O and PA changing from 15 to 30 cmH2O when the lungs were normal and after they were made edematous. When Pvas = 2 cmH2O, increasing PA increased the Vvas and the FFR in both normal and edematous lungs. However, when Pvas = 10 cmH2O, increasing PA only slightly changed the Vvas and reduced the FFR in the normal lungs, and decreased Vvas and markedly decreased the FFR in the presence of edema. Inflating zone 1 lungs by positive pressure has an effect on transvascular fluid flux that depends on the Pvas. The results suggest that the sites of leakage in zone 1 also vary depending on Pvas and PA.